Okay, okay, let's get started. I have an announcement before this last talk of Nati. This afternoon is going to be a special session to felicitate the physics contributions of Kumar Narayan who is one of the main organizers, who has been one of the main organizers of the school for the last 25 years. I urge all of you to attend it. It will give you a perspective on the history of strength theory a little bit, and also the more classical period of strength theory when the world sheet was important, modular inverse was important. So you haven't heard anything about that during this school, but this session will give you kind of a new, different perspective about strength theory. So I encourage everybody to attend it, and now we'll start with the last lecture. So even though they updated it up there, they still insist that I give the same talk that I gave yesterday, but I will not. What's that? It will be what? Okay, I can do that. I have no problem. I'm about the end of lecture two out of four that I planned. So I'm not going to finish my notes anyway. I need more chalks, longer chalks. Okay, good. So yesterday, we discussed something bad with the sound, with some feedback. There was, we started discussing dualities and we discussed particle vortex duality and just by manipulating the standard particle vortex duality, we derived the new boson boson duality, which looked a lot, this theory that we studied was a gauge Wilson Fisher model that we denoted like that and I'll symbolically write it like that so that I tune the coefficient of phi square to zero and what I really mean by that is no symmetry at the point phi square equals zero. So what I really mean by tuning is that I tune it to the fixed point of the infrared theory and different people might have different regularizations and then what they mean by mu square in the Bella grandeur would be different but what is meaningful is that there is a fixed point and what I call mu equals zero is being at the fixed point. So this way, if you and I have different regularizations and you define your mu one way and I define my another way, once we found the fixed point we can both adjust what we mean by mu such that mu equals zero is the fixed point. So I did not include it. Also the coefficient of phi to the fourth will let it flow all the way to the infrared. So it's no longer a parameter in the theory so I'll denote it schematically by one but what I really mean is that we start with the Lagrangian as last time. With the phi square in with the phi to the fourth we flow to the infrared, we tune mu and we call that mu equals zero. So this is shorthand for all that and we also said that we add here i over four pi bdb. So it's not just the Wilson-Fischer fixed point coupled to a gauge field with a chance simons level one and we added to it coupling to background field two pi bda. So this is what you really mean by that is this theory in the UV that there might be a gauge coupling for b and there might be a mu term and a lambda phi to the fourth and we flow to the infrared and we look for the fixed point. We readjust what the parameters are and in the end we have this theory that doesn't have a free parameter. It has a global U1 symmetry. A is our device to probe the global U1 symmetry. It's a classical field and the claim yesterday was that this whole thing in the infrared is the same as a free fermion coupled to the same background field psi. So in the past five minutes I fulfilled the requirement of the organizers that I would give last talk and I also the requirement from here or the request that I give it again. So now we can proceed and what we'll do now is use another trick which is the same trick essentially that we use yesterday that once we have one duality we can plug it in and do the same manipulations on both sides and derive many other dualities. So again, we have this duality. Recall we derived the boson, we started from a well-established boson boson duality. We actually derived from it another boson boson duality which is essentially this theory with some signs flipped and some added term, classical terms. And then we said this looks like a fermion so that's an assumption. We are going to assume this duality and now I'm going to derive consequences. For the rest of the talk I will just derive consequences of this duality and I'll derive many other dualities and we'll present checks on the other dualities and if any of them fails it would mean that this duality is wrong. As long as they are checked then this gives us more confidence in this duality. It did, it did, it did. So there's a question of whether you mean the particle or the operator. I'm answering your question. So you could mean two different things in the question. One is what is the map of operators? Can somebody sitting in the UV in the bosonic theory identify an operator's side? That's a way to interpret your question. So let me answer that. In fact I did it yesterday. I say that on this side of the duality we can consider a monopole operator for B. It's not a soliton. It's a monopole operator and because of this term it is charged under the u1 symmetry of B. So we multiply by phi or phi dagger depending on your conventions. And we argued yesterday that this is mapped to the operator's side. So in the UV you can really see the operator's side. So even in the UV here where the theory is interacting and complicating you can see that it has an operator which has spin a half. It's a fermion. It carries charge one under the u1a symmetry. But it's not free. So in the UV I'm trying to answer your question. So there is such an operator in the UV it has spin a half and charge one and it satisfies a very complicated equation of motion. Claim is that in the infrared the equation of motion of this fermionic operator is that of a free fermion. That's a non-trivial dynamical statement. The fact that there exists an operator of spin a half and charge one that's easy to establish and that's true in the UV here. The claim of the duality is not that this theory in the UV is the same as this. It's only the infrared is the same. So we identify this. Another way, let me finish this and then you can ask your question. Another way to interpret your question is about states in the Hilbert space. But one thing at a time. This thing has been going on for some 30 years. When there was still in Russia and I had not seen him we had a very long email exchange and it took three weeks each way with long letters written long long hand and the style was exactly like this. And I was younger. I don't know whether he was younger than or not. So another way to interpret your question is about the states. So the operators are always defined in the UV. They are independent of what the parameters are and so forth. The parameters determine which phase the theory will be in. They determine the spectrum in the infrared. That's a separate question. So let's discuss the parameters and the phases. So we said that the operator psi bar psi is mapped to the operator phi absolute value square or maybe with a minus sign. Doesn't matter. So that's still in the UV. This is the map of operators. Now we discuss states. In order to discuss states we need to know which phase we are in. And we discussed yesterday three phases. One is mu equals zero. That's a transition point where this theory has a fixed point and this theory has a fixed point. In this language the fixed point is a free field theory in this language we don't know and the claim is that it is free. At that point the states are massless particles so it's very confusing what we're talking about. So we should better be in one of the other phases to formulate your question precisely. And there are two phases depending on whether mu is positive or negative. In this side of the duality when mu is positive we have a fermion with positive mass and when mu is negative we have a fermion with negative mass. And they each have spin a half and they either spin this way or that way because we are in two dimensions. And there is an anomaly that tells us that these two states are not exactly the same. But there is one free massive fermion. Now we go to this side of the duality. And now I'm getting closer to your question. Can I see this state not operated fermion that I see here? And I explained yesterday that depending on the sign of mu the answer here is different but in both cases we see a fermion. For one sign for positive sign the spectrum includes five quanta. They are five particles. The five particles are the excitations in the spectrum. Mu is positive, make it much bigger than anything else. You have five particles. But the five particles are charged under little b so we have to be a little bit careful about them. And little b is a gauge field which was not Higgs so its dynamics is important and it has churned Simon's term. A massive scalar field coupled to a churned Simon's term acquires fraction of spin and fraction of statistics. So phi itself acquires spin-a-half and therefore it's a fermion. And we can also check that it has a charge one under big A. In the other phase it's even closer to your question because in the other phase what happens is that phi condenses. Once phi condenses two things happen. First it Higgs is the gauge symmetry. From this point on all the subtleties with churned Simon's terms are not present. But what we get in return is that this is the Abelian-Higgs model and it has vortices. Which I think were mentioned in one of the talks yesterday maybe even yours or maybe Misha's. These vortices are strings in three plus one dimensions and they are particles in two plus one dimensions. So this system with negative mu has vortices. And if you go through the analysis there you see that these vortices have spin-a-half and charge one under big A. So they have precisely the right quantum numbers to be the free fermion in the other description. Now you can ask your question again if I did not answer it. Okay, thank you. Okay, so this is officially now the end of lecture three. And we are going to manipulate this duality. And the trick of manipulation will be exactly the same as we did yesterday. And this is the main trick in this game. So we are going to add terms to the two sides of the duality and convert A, the classical field to a dynamical field. And specifically the theory we would like to understand this is a free fermion coupled to a classical gauge field. We would like to study three-dimensional QED, namely a fermion coupled to a gauge field. So once we have the duality we'll be able to give a Bosonic description of this theory because wherever we see psi with a covariant derivative we'll just use the right-hand side. So let me do that. So I'm going to add to the two sides of the duality. I'm going to add I over two pi, ADB. And whenever we add a new gauge field we can add. So the idea is to promote A to be a dynamical field. So whenever we have a dynamical field we always have a classical field coming together with it that couples to it like that. And we also, nobody can stop me from adding one over four pi BDB. You will soon see why I did that. So we just add that to the two sides of the duality. So the duality is like an equation. We can add the same thing on both sides. So it's still true. And here it's trivially true because these are classical terms. They don't affect the dynamics at all. Now since the duality is true for every A I can integrate over A. So the way I do that is by replacing A by lowercase A. So on the left side of the duality I have this. That was there before. And I'm adding I over two pi. And B is now a new classical field. So I've just done that. So this is QED coupled to a classical background field that for some reason has a BDB which so far it looks totally unnecessary. On the other side of the duality we have many more terms. So let me copy. Have that. Now we have plus I over four pi BDB plus I over two pi BDA. There's something wrong with my signs I think. That's okay. Plus I over four pi sorry one over two pi terms I added there. That now A is going to be a little A. I added a DB plus I over four pi. So what have I done? I added this thing to the two sides. And wherever I saw big A I replaced it with little A which is shorthand for I'm going to integrate over A. A is going to be a dynamical field. But now we can do the same thing we did yesterday. We look at the terms in A. So the terms that A multiply A appears only linearly on this side. Since A appears linearly it's easy to integrate it out. So the general rule is that whenever we have e to the I minus I over two pi A dx. X is whatever it is. Then the functional integral over X gives us a delta function of delta function integral over A gives me a delta function of X. This is a trivial theory. You can think of it as being a Lagrange multiplier that forces X to be trivial. So if I just look at these terms they tell me that B is minus B. Right, but with the coefficient here so what does it mean? It's clearly a delta function of the derivative. It means that dx is zero. That's obvious. But I claim that it really means that X is a pure gauge. So dx equals zero is weaker than saying that X is a pure gauge. I also need to worry about the holonomies but that depends on the specific normalization. Since A is not really a number but it's a connection then A might not be single value. So that might be, I might need transition functions in A and when I integrate over these that really sets X to be zero and what I mean by that is a pure gauge. So that was a good question. And so now I can integrate out and I forget about this and I can forget about that. And I can also forget about little B because it's the same as plus B. So these two terms cancel. This becomes big B and I might have messed up a sign but oh I see my mistake. I had a minus sign here yesterday. Quality I wanted. So with this minus sign I have it here. So now B is minus B. I can cancel these two terms and what I'm left with, so now I'll do it on the blackboard, this theory with a lot of fields boils down to up to redefining what I mean by B, dB pi square plus pi to the fourth and everything else cancels out. So what do we see here? On the left hand side we see QED, a theory which is also known as U1 level a half because of the parity in number. This is a standard theory that there is huge literature on it with different number of flavors and there's really huge literature on that. And on the right hand side, we find the Wilson Fisher or the O2 Wilson Fisher model or the XY model. This result is extremely surprising. It's extremely surprising for a number of reasons. First of all, QED in three dimensions, so forget the coupling to B for that matter, just a free fermion coupled to a gauge field is a strongly coupled theory and it is controversial what this theory does in the infrared. In fact, lattice people have not yet converged on what it does. There are people who claim that there is a first order transition. There are people who claim that sidebar side gets an expectation value. We have a claim here. I don't might not be right, but the claim is very specific. This theory has a second order point. It's a non-trivial fixed point and not only is it a non-trivial fixed point, it's a well-studied, well-known fixed point. This is the XY model. That's the first reason this is surprising. There's a controversy in the literature of whether such a fixed point exists at all and we claim not only does it exist, it's a theory that everybody is familiar with and if you're not familiar with the XY model, you should be. This is a well-studied model. It describes things in nature. There are measurements in the lab measuring the critical exponents of this fixed point. This is well-established with the transition of superfluids and so forth. It's exactly the same fixed point that this controversial theory flows to. It's a very specific statement. Number two, QED, whatever it is, is claimed to be a theory that is not time reversal invariant. For classical A, there was this Tuft anomaly, which means that the free fermion is time reversal invariant for any classical, for zero A, but with non-zero A, we had this anomaly and it wasn't really time reversal invariant. When we integrate over A, we cannot avoid the question of what happens when A is non-zero because we integrate over this and that means that the theory is not really time reversal invariant. So three-dimensional QED, with one flavor, is not time reversal invariant. That's a statement. What does it do in the infrared? We claim that this is the same as the Wilson-Fischer theory, which is time reversal invariant. So the claim that this is not just a fixed point, but it's a known fixed point, is even more surprising because we start from a theory in the UV that does not have time reversal symmetry. In fact, that's the canonical example of a theory where time reversal is anomalous. So you start from a theory that classically has time reversal symmetry and you go through a long discussion arguing that it's actually not time reversal invariant and at the end of the day, it does become time reversal invariant but with a different time reversal transformation. The time reversal transformation or the time reversal symmetry in the infrared is not the same time reversal that we saw in the UV that was violated. So the theory in the infrared has a new time reversal symmetry that acts locally on the fermion side. Question. These are massless fermions. Let me clarify your question. In general, when you want to say something is massive or massless, there is a natural way to discuss it. When the particle is massless, there is an enhanced symmetry. So you don't just declare what the parameters are because what the parameters are can depend on your regularization, the way you define the theoretical distances. You use Pauli-Villas or dimensional regularization. You put it on the lattice one way or another. What you mean by mass could be different. But if there is a point with enhanced symmetry, you could say, aha, what I call m equals 0 is the point with enhanced symmetry. So you and I have different regularizations. What you call the mass is not what I call the mass.  That is known technically that this is a natural definition. Now, in this theory, in the free fermion theory, it's more tricky because the point m equals 0 does not have an enhanced symmetry. There's no enhanced symmetry at the point m equals 0. And therefore it's a little tricky to say, what do you mean by m equals 0? There's no special symmetry. So I'm going to define m equals 0 as the point where there is a transition. This theory clearly has a transition because for mass positive and large, we have a fermion in the spectrum with positive mass. And for mass negative and large, we have a fermion with negative charge. So there must be a phase transition between them. I call m equals 0 the point of the phase transition. Now we can communicate because we define what we mean by m equals 0. And then m equals 0, we claim, is a second-order point. It could have been a first-order point, but at least we know what we're talking about. So the claim here is about m equals 0. Now, for the free fermion, this parameter m, or we call it mu, breaks time reversal symmetry for the free fermion. In this theory, since we integrate over the gauge field, there isn't even such a symmetry. So there's no symmetry at this point. And indeed, if you go through the change of variables that I did here, the fermion mass from here is mapped to the boson mass here. And the point mu equals 0 in this case, so let me write it explicitly. So psi bar psi is mapped to the operator phi absolute value square. And indeed, in this theory, mu equals 0 is not any special as far as symmetry is concerned. Mu equals 0 in this side is characterized by having a transition at that point. There is no symmetry that is enhanced at that point. And similarly, on the left-hand side. So this is... If it's second-order, not still. If it's second-order, it is... No. I would call mass 0 when there's a particle. When there's a particle, I know what the mass means. This theory is not free. In lecture 3, which spilled a little bit to the beginning of this one, the mass was meaningful because the theory in the infrared was a free theory. It was a free fermion. Now, the theory in the infrared is interactive. So the notion of mass is not well-defined. There's no mass of particle. There's a parameter in the Lagrangian. No, there's a deformation from the fixed point. And it is what it is. It is irrelevant in the infrared. So it's relevant in the UV. The kinetic term or the Chern-Simons term? The kinetic term is a relevant operator in the UV. It dies in the infrared. So we get 1 over g squared times db1ad square. And as g becomes big, 1 over g becomes small. And in this shorthand notation, I send it to 0. So you see, if I wanted to write the full Lagrangian, there would be more terms here. There would be 1 over g squared and db on this side. And on this side, there would be 1 over g squared. No, sorry, a. And on this side, there would be 1 over g hat squared times db squared. And there would also be mu at mu squared and pi squared. There would also be a fermion mass here that we tuned. So there are all sorts of terms that either flow to 0 or we tuned them away. And in order not to write too many terms, I did not bother to write them. So this is shorthand notation. What we really mean is a UV theory with all possible couplings. We flow to the infrared. And after we flow to the infrared, we either do not write them or write them the way they are, or there are parameters that remain relevant in the infrared. So these are all the irrelevant parameters in the UV. I just don't bother to write them. And all the relevant parameters I tuned to a fixed point. So they're still a parameter. I need to explore the deformation. But we would still like to map the operators, because this is a very dramatic claim. So in order to make it more palatable, we would like to map the operators in more detail. Because I was asked about it. But before we discussed the bilinear, we would like to ask, where did the fermion come from in this theory? This theory has no fermions. And conversely, where is the order parameter phi, the order parameter for the U1 breaking in the fermionic language? So I'm going to answer these two questions. And let me start from the fermionic theory. In the fermionic theory, this is QED. So it has a dynamical gauge field. Whenever you see a dynamical gauge field, you should start in monopole operators. So this is a monopole operator for A. And the monopole operator for A, just by looking at this term and integrate by path, we see that the monopole operator is charged under B. So it's an operator, it's a scalar operator, carries spin zero, and it is charged under B. In this language, there is such a guy, which is phi itself. So we identify the monopole operator in B with phi itself. What about the fermion? This theory has a fermion. Should we identify it with anything in the bosonic theory? That's a question. Well, we don't have to. It's not gauge invariant. Thank you. So operators that are not gauge invariant, either we can multiply them by something else to make them gauge invariant, or we don't discuss them. So in this case, previously the fermion was gauge invariant. So we had to do a double symmetry coupled to the classical field A, so we had to discuss it. Now the fermion couples to a dynamical field, and therefore we don't need to discuss it. So what do we have here? We have a theory that has a U1 symmetry acting on the local operator. We identified it on both sides. There is one relevant operator, so this is a relevant operator and there is another relevant operator that does not carry any quantum numbers, and it's this guy. So we can relate them between the two sides. We can also consider deformations by... Oh, I'm behind in time. We can consider deformations by the relevant operators. That's somewhat less interesting to do turning this guy on because it breaks the symmetry. So let's preserve the symmetry and turn on this guy. So now we are going to have massive QED on one side, and the Wilson-Fischer fixed point on the other side. So for the case of the bosonic side, we've already analyzed it before. This theory with positive mass, the U1 symmetry is unbroken, and since it's unbroken, there are massive particles, the phi quanta, which sit there and there are massive particles. In the other phase, the global U1 symmetry is spontaneously broken, and there is a massless goldstone boson. I am not going to do it in detail here, but the same thing can be obtained here by considering the fermion and giving them a mass. So that leads to the same answer. So what we have seen is that... What we have seen is that we derived a new duality which answers a long-standing question. What does QED in three dimensions do? And the answer is something we already discussed before. So that's new. To learn about the new quantum field theory. And this identification has passed some elementary tests. There are more tests that I'm not discussing here today, but they are in the literature. So that's what I wanted to say about this duality. But in a similar way, we can easily construct more dualities. So we could start, for example, from here. Let me erase all the irrelevant stuff. We don't need all this. We don't need all that. So this is QED. So it's a fermion with a dynamical gauge field coupled to a classical gauge field in some term. And that's just a purely bosonic theory. Once we have this duality, we can easily create more dualities in the same spirit I've done before. So, for example, I can add to the two sides of the duality I k over 4 pi bdc plus sorry, plus i over 4 pi this is 2 pi because it's off diagonal, this is diagonal, i k over 4 pi bdb. So I can add this term to the two sides of the duality and then declare that big b is little b, i.e. I'm going to integrate over it. I'll manipulate the two sides and I'll find something. And that something might not be interesting. I might be able to do it a few more times and generate many more theories that I can analyze this way and generate many more dualities. So this is a lot of fun because this is really a machine that spits out dual pairs. And you have to be careful when you do that not to make mistakes and be careful about the plus sign and the minus sign, etc. And a lot of that has already been done. But this leads to a whole set of new theories. So let me give you an example. And I'm not going to do the algebra on the blackboard because I've already done it a few times in these lectures. But let me write one example so I can have one i psi bar d slash psi and you can take it as an exercise for you to work out. It's really not a lot of work. I over 4 pi a plus i over 2 pi a p plus i over 4 pi c dc and I can even add the gravitational trans-simon that I suppressed before. And that's dual to b of i where plus 5 to the 4 the same as before minus 2i over 4 pi pdb plus i over 2 pi so let me say it in plain English or in words. The theory on the left hand side is QED namely a fermion, a single fermion coupled to a gauge field and that gauge field has a u1 before we had u1 level a half. So this has a half buried in it but now we add one more from here so this is u1 level 3 halfs and it's coupled to some classical fields that we can suppress. So this is a cousin of QED this is the same QED but the gauge field also has another trans-simon term. We could be interested in this theory with an arbitrary coefficient here. It would be u1 with an arbitrary k. Yes. Which level? There's no k here. I added something like this with an appropriate k. I think you get this thing for k. If you take this thing I think with k equals 2 either 2 or minus 2 you will land on this. I think it's minus 2. Well there's a question of whether you edit or subtract it and there's some missing the minus signs in my notes so I shouldn't say but it's either 2 or minus 2 and you will land on this. I'm happy to do the algebra on the board if you want but this is really straightforward algebra and it's identical to the algebra I did for twice. Once when I did this trick of adding such terms to the two sides of the particle vortex duality and then I did it again this morning to derive QED. So it's identical to that and in general you can do it with an arbitrary coefficient here as long as you do it on both sides and you end up with this. This was changed because of k. So we end up with u1 level 3 halves so the naive QED has level half it always has to be half integer and now we add one more so we have 3 half. This is another theory we could be interested in and people have been interested in this. QED with any number of fermions with various levels for the chair and Simon's gauge fields is used literature on the subject I think even Spenta wrote on that if I'm not mistaken. Yes or? The non-Abelian that's also interesting we can discuss the non-Abelian one. So this theory is huge literature on it and it couples with some background fields because it has a global u1 symmetry so we can couple it to C and the claim is on the other side this is again the Wilson-Fischer theory but it's a gauge version so it's coupled to u1 level minus 2. So both the theory on the right and the theory on the left a theory is that there was an interest in them. The Wilson-Fischer theory can be gauged and once it's gauged it can be coupled to a trans-Simon's term and again people have discussed that in the past here the fermionic theory is QED so it's already gauged and you can add a trans-Simon's term to it this has been discussed in the past and one might think okay we have two separate theories but the duality claim is that this theory is the same as that one so we put some order in this long list of possible fixed points in three dimensions by identifying some of them some of the line operators can be mapped and some of them cannot be mapped and in order to see those that really carry meaningful information as far as global symmetries can be mapped those that do not carry such meaningful information do not have to match on the nose in general you can map even for local operators operators that are charged you have a charge operator here charge operator but then only those that are kind of the lowest dimension charge operator because the others can mix and you should also be able to map the relevant operator because they tell you where you go and the renormalization goes through the irrelevant ones are getting trickier yeah in supersymmetric theories you can do better but here we don't have supersymmetry so you cannot do better yes in the first one is it no yes in the sense yes it's a good question but the answer to the good question is no there are two kinds of things in infrared so duality is divided into two kinds first exact dualities example N equals 4 super young males another example the icing model with Kemevenia duality that's first class class number 2 are infrared dualities and in infrared dualities they are again further divided into two categories category 1 you have two different UV interacting theories that flow to the same fixed point case number 2 one UV theory flows to another and that's meaningful when this thing is infrared free the distinction between them is not sharp so for a given theory the distinction is sharp but if you start making deformations it's not sharp so imagine you take something like this and you add a relevant operator to add here a relevant operator now this one might flow to a non-trivial fixed point and this one will have to flow to the same non-trivial fixed point because of the duality but now you say that this and that flow to the same infrared fixed point so it looks more like this and you could also go the other way around with appropriate deformations so what do we have here here we have a fermion so we have a free fermion coupled to a gauge field and the relevant coupling here is the gauge coupling so the relevant coupling here is the gauge coupling and here it's the Wilson Fisher theory the relevant couplings are the 5 fourth in the gauge coupling and the non-trivial claim is that they flow to the same point I'm not going to do it here but I want to mention that all these dualities are the generate cases of a much richer structure with non-abillion gauge groups so you can repeat the same story with non-abillion groups so you have some fermions and they couple to some SUN and you have some bosons and couple to some UN and you can have transimons so there are now lots of knobs that you can turn changing the gauge group it could be an orthogonal group or a unitary group and you can change the transimons level of dualities between them and there are lots of cross checks so this is a very rich subject and one of the conclusions from this rich subject is that this particular theory which I presented two dual descriptions really has more dual descriptions with non-abillion groups so here Spenter should get the credit because he did study these theories with non-abillion groups so for example this particular example is the same as a fermion or QED or just straight fermions couple to SU2 level a half and a half is again because there is a single doublet and it's also dual to another theory which is the Wilson Fisher theory couple to SU2 level minus 2 A minus 1 so lots and lots of dualities so lots of theories that you could just be interested in bosons fermions couple to this gate group that gate group with different levels and they all can flow so these theories are totally different in the UV they have different degrees of freedom different symmetries and they all flow to the same infrared fixed point so we have already discussed the fact that this theory and this theory flow to the same infrared fixed point what's the global symmetry here what's the global symmetry of this theory we've discussed that my presentation there was a classical background field that coupled to it it's this theory it is coupled to a classical background field what letter did I use for it well that's it's not a level because it's a classical field it's U1 so this theory has a classical U1 symmetry actually to be precise it's O2 because there is also charge conjugation this theory this theory is this one also has a classical U1 symmetry magnetic symmetry so this one also has a U1 but if you write the global symmetry you write the Lagrangians here you will see that these two theories really have an SU2 global symmetry or more precisely SO3 so these theories have an SU2 global symmetry and the non-trivial dualities tell us that they flow to the same point so I haven't done that in these lectures I'm just stating the fact I'll soon make it more plausible so the interesting statement is that these two theories that we were discussing before have a global U1 symmetry and they flow to a fixed point that has an SO3 global symmetry we have seen a lot of that in two dimensions if you have a compact boson in the radius the global symmetry is U1 or U1 for the left-movers and U1 for the right-movers as you change the radius there is a quantum symmetry the global symmetry becomes SU2 and it actually appears twice once SU2 for the left-movers and one SU2 for the right-movers that's well known that's I don't know 70s or 60s even before my time there are two dimensions in supersymmetric theories there are theories that in the UV have a U1 symmetry and in the IR have an SU2 symmetry that comes under the title of three-dimensional mirror symmetry now we see the same thing in a non-super symmetric theory so let me make it a little bit more plausible and give you some more insight of where this thing comes from so the various theories we discussed are various, the Wilson Fisher the O2 Wilson Fisher fixed point and it could be coupled to a U1 gauge field and the U1 gauge field could have various levels so the simplest one which appeared yesterday it was the Wilson Fisher fixed point coupled to a gauge field no chance, Simon's term at all this theory we showed in the first lecture is the same as the Wilson Fisher fixed point without gauge fields how is this duality called? this is the duality between the 5-4 theory and the 5-4 coupled to a gauge field we gave it a name we didn't give the name, the name was given by others I repeated the name that's particle vortex duality that's known from the 70s today we'll learn that this theory is also the same as QED this theory is the same as QED and the natural order parameter is the monopolar the monopolar operator from here and that was mapped to the scalar field of phi scalar field phi of then we also discussed the Wilson Fisher theory with U1 level 1 so we take the same theory we have a gauge field without a trans-Simon's term it's the same as the Wilson Fisher theory now we add trans-Simon's level 1 this theory is also dual to a theory that we like what is it? give you a hint somewhere on this blackboard well it is on the blackboard this one, no this is QED level 1 half look at the far end of the blackboard it's the free fermion and the monopolar operator is mapped to a fermion now the monopolar operator requires spin because of the ADA type coupling or the BDB type coupling in the Lagrangian and the monopolar operator we said always has so the monopolar operator if we have K BDB 4 pi the monopolar operator has spin K over 2 that appeared in the first lecture appeared in the second lecture this is the spin of the monopolar in this general Simon's theory so for K equals 0 we got a scalar which we identify with this scalar for K equals 1 we get a fermion spin a half which we identify with the free fermion and now we are discussing the Wilson Fisher with U1 level 2 or minus 2 it doesn't matter and we found many dual theories what's the spin of the monopolar operator in this theory 1 so what can an operator of spin 1 be what other operator of spin 1 are you familiar with a master's vector field is not gauge invariant but an operator of dimension of spin 1 which operators have spin 1 the quantum field theory that has I'll give you a hint it might be conserved conserved current so the monopolar operator of this theory is mapped to a conserved current so it is an operator of spin 1 in the UV because there is such an operator in this theory but it's not conserved by the time we go to the infrared its dimension goes down it becomes conserved and it combines with the global U1 symmetry that we see with the naked eye so by looking at the UV we see a U1 global symmetry this is the magnetic symmetry and we see that the lowest dimension operator charged under that global U1 symmetry has spin 1 this doesn't mean that it's conserved and therefore it doesn't mean that there is an SU2 global symmetry but it does mean that as we go to the infrared its dimension could go down and it has the potential to become conserved and the claim of the duality is that it is indeed conserved and there is a global SU2 symmetry I've already mentioned the analogy between this and the two dimensional problem in two dimensions when we have a compact boson there is a global U1 symmetry the shifts x shifts x by a constant and there are winding modes and the winding modes carry charge under that U1 symmetry and for large radius and for large boson the winding mode has very high dimension but as we crank the radius down the dimension of this winding mode comes down until it hits dimension 1 which is the dimension of a conserved current and at that point the global symmetry is enhanced to SU2 this is well well understood it's known as the Frankl-Katz construction and it appears in string theory all over the map I haven't studied that I strongly encourage you to study this what we see here is a three dimensional cousin of the same phenomenon but it's much more interesting because it happens in an interacting theory whereas in two dimensions it happens in a free field theory and this phenomenon in interacting theories in three dimensions was also known in the supersymmetric theories in supersymmetric theories you often have a global symmetry and in the infrared these U1s become the carton sub-algebra of a non-abillion group and the extra elements that enhance the abillion group to a non-abillion group come from monopole operators so this is well understood in supersymmetric theories and now we see that the same phenomenon happens even in non-supersymmetric theories and now you can ask your question which vector boson? When you said that it was interaction with gauge field I called it vector field so now you have a partner to raise this field to non-abillion one so in this sense I'm wondering like I think you're mixing two different things think number one in this theory there's a dynamical U1 gauge field this dynamical U1 gauge field is not associated with any symmetry because whatever it couples to is coupled to a gauge field and therefore it's not a new global symmetry even that we have a U1 gauge field which is dynamical it's not true for classical gauge field is its own conserved current a quantum gauge field like this one it couples to a conserved current but there's no global symmetry instead there is a monopole operator and there is a magnetic symmetry so whenever you have a dynamical U1 gauge field there is a global U1 symmetry associated with it but it's more subtle the conserved current is f mu nu so that is the U1 that is being enhanced the U1 that is being enhanced its current is f mu nu but in terms of states do not appear remember you answered it's the same question you can either discuss states or you study operators when you ask what's the symmetry you ask about operators when you ask how it is realized in the Hilbert space you ask about states that's a different thing the question of what the operators are that's something that you see in the UV it's independent of the dynamics independent of the theory that we have phase transition there would be a superconductor we don't care when you discuss states you should analyze it separately for each value of the parameters especially when they are phase transitions different phases the symmetry might be realized differently for example it might be spontaneously broken or it might not be spontaneously broken so for any one of these dualities you can turn on various mass terms positive or negative and analyze semi-classically what the spectrum looks like and hope that you would be able to land on your feet namely if you see a massive spin zero particle here with some charges you go to the other dual description and again you see the same particle so for particles it's a separate question and in this case we can ask is the symmetry spontaneously broken etc etc in this description the new symmetry so the u1 is there the global u1 where was my diagram this global u1 is there everywhere and the monopolar operators are charged under it and the particles in the various phases are charged under it there is among other things a particle in some phases in the phase where this u1 is unbroken there are massive particles with spin 1 that's a massive particle it has spin 1 not a conserved current, no nothing there is no su2 symmetry there is no su2 global symmetry the statement about the enhanced su2 symmetry is only about the infrared not about taking the uv theory and turning on masses so when you want to discuss particles that's a separate question and here in the uv it's not going to shed any light on it having said that we can discuss these two theories in these two theories the full su2 is visible in the uv and therefore in each phase of these the su2 should act either should act on the spectrum if the su2 is unbroken or be spontaneously broken and there will be goldstone bosons so you can analyze all that and it has been analyzed and it actually works but you see there are many theories and many parameters so there is a lot of work to do and it was done okay I reached a natural point to stop and I really said a tiny fraction of what I plan to say well give about a half of what I plan to say and it is a tiny fraction of what is already known about these dualities but I hope I gave you the necessary background to read these papers things that are hard to find in the literature like the proper statement of the anomaly and some introductory comments on Chairman Simon's theories which allow you to read the papers I should just mention that we discussed boson boson dualities that is known from the 70s yesterday and today we discussed boson fermion dualities and you can iterate these and find also fermion fermion dualities so that is one direction you can take you can also change the gauge group in all sorts of different ways you can also change the potential if you have the gauge group it is sufficiently complicated you have enough scalars instead of having just one scalar you have several scalars and then you can write different terms in the potential that break the symmetry there are different global symmetries and there is a very rich structure of fixed points that you can find or might not have some dual description using totally different degrees of freedom so it is a huge zoo of examples that can be studied and some of them already have applications in condensed matter physics in fact some of these things were motivated by applications in condensed matter physics some of them were actually done by condensed matter physicists not quite in this language so I feel that there is a lot that can be done I even prepared here a lot of things that I did not cover and I hope that the young people in the audience could take it up and push it forward so stop here


Unfortunately, that is all the time we have for questions. It's now time for member statements. I recognize the member for AJAX. On February 27, Calgary welcomed athletes from across the country to the Special Olympics Winter Games. I am honored to rise today to recognize Ella Robinson, Alex Capucci, and Rebecca Osman, three competitors from my constituency of AJAX. The Special Olympics provides athletes with intellectual disabilities, an incredible opportunity to showcase their talents and shine in a world that can often be challenging. Through these games, barriers are dismantled and new heights are reached. The accomplishment of these three champions are a testament to this as they collectively brought home a total of nine medals. Ella secured first, second, and third place in three race categories. Alex, impressed with bronze medals in all four of his speed skating competitions. And Rebecca added to the team's success by placing second in five pin bowling. As we watch Ella, Alex, Rebecca, and all these athletes experience a joy and camaraderie of victory, we are reminded that this event transcends the boundaries of playing field. Mr. Madam Speaker, it is an event that forms a community and fosters friendships for that last lifetime. My heartfelt congratulations to Ella, Alex, and Rebecca for representing AJAX with strength, unity, and determination. A special thank you to Donna Edwards, who has been an amazing coach and leader in Special Olympics for many years. For the member's statements, I recognize the members of London North Centre. Speaker, I recently had the opportunity to tour Arcade Street Mission's Chrono Warner site. I'd like to applaud the City of London and all of the phenomenal service and community partners working on the whole of community health and homelessness strategy tables. It was rather cold as we walked down Dundas Street from Arcade's main location, punctuated by our entry into the warm Chrono Warner location. I want to thank the diocese of Huron and the Board at Warner Place for providing the location at a fraction of the market rate to care for the marginalized people in our community. Arcade has served 900 unique people this year. We heard from Rob, who struggled with accessing health care while homeless. He was proud to tell us about his improvements and his future goals. None of this would have happened without Arcade and housing. But funding for these spaces and others like Safe Space and many more will end on May 31st this year. Homelessness in London will not end on June 1st, Speaker. If funding doesn't flow, 100 dedicated and caring staff will be unemployed. 120 resting places will become vacant, vital and necessary. I was shocked to learn the providers will have to warehouse all the mattresses while people sleep rough. I call on government members to listen to their conscience and fund these beds now. Think of the people who are rebuilding their lives and whose hopes and dreams will be much further away without the basic human necessity of housing. We have the space. We have caring people ready to help. All that is needed is political will. Housing is foundational. Housing is fundamental. Housing is a human right and housing is health care. Thank you, Speaker. Further member statements? I recognize the member for Lanark, Frontenac, Kingston. Thank you, Speaker. Speaker, Ontario's 2024 budget revealed this government's plan to rebuild the economy while continuing to invest in health care, housing, infrastructure, and more without raising costs for families. In long-term care, the $155 million in funding in 2425 will allow for continued progression on building 58,000 new and upgraded long-term care homes, long-term care beds across the province, like the completed homes in Carleton Place and Almonte, and the broad-view long-term care home in Smith Falls currently under construction. We're investing just over $3 million to assist up to 3,500 people in connecting to primary care in Perth, Ontario, and 4 million to help up to 10,000 people at the Parawinkel site in Kingston. This budget also greenlit the reconstruction of Princess Street in Almonte and the reconstruction of Battersea Road in South Frontenac. Speaker, access to high-speed internet and mobile service is a necessity of modern life, and that's why we're investing $71 million through the Eastern Ontario Regional Network to continue getting more communities online faster than ever before. These are only a few of the highlights of the 2024 budget that is supporting economic growth in Lanark, Frontenac, Kingston, and across Ontario. Our government is committed to creating stronger communities for the future, improving Ontario's productivity growth, and building prosperity for generations to come. Thank you, Speaker. Thank you very much. Member Statements, the Member for St. Catharine. Thank you, Speaker. In Ontario, yesterday, acknowledgements that interpartner violence is an epidemic. Spurred by Ontario's NDP Bill 173 is a step forward. It is encouraging to see the government finally support this recommendation. However, the results must be genuine action, not more delay tactics. 18 months ago, I urged the government to review and to act on the Renfrew triple thymicide inquest. 86 recommendations to eradicate this violence. Leadership is about facing these truths, and the truth is the government is acting too slowly. This conservative government has a plan by experts that has been on their desk for over two years. It is concerning that the government committed to an in-depth study. The time for studies is over, the time for action is now. In Niagara, we endured a tragic femicide only a few months ago, and while we have the best service providers anywhere in the world, they need our help right now. We need immediate, robust solutions, education and training within our criminal justice system, comprehensive and permanent funding, bringing forward an Ontario glares law, and securing funding for survivor services. Let us honour those who have suffered and those fighting for change by committing to immediate, decisive action on gender-based violence, not another study and not another delay. Thank you very much. Member Statements, the member for Burlington. Thank you, Speaker. Once again this year, I have the pleasure of attending Halton Industry Education Council's 20th Annual Women as Career Coaches Mentorship Event. Congratulations to the team at Hayek for reaching this milestone and for your continued efforts in bringing together women and mentors. For 20 years now, this annual event has brought together young people and adult mentors for an impactful, inspiring and uplifting evening. During the evening, guest speakers share their career journeys and advice with youth who are just starting to think about potential careers. Career coaches sit at tables with young women engaging in lively conversations, answering questions and offering encouragement. Throughout the evening, a lineup of inspiring speakers talk about their journeys and career paths and youth have an opportunity to participate in panel discussion. This evening is designed to, the evening is designed to provide the next generation with the opportunity to discover a wide range of potential career paths and perhaps think about new career opportunities. Speaker, working together, we can inspire youth to feel confident and optimistic about their futures and their place in the world of work. Thank you. Thank you very much. Member Statements, the member for Spadina, Fort York. Thank you, Mr. Speaker. In the early 1990s, I was a teacher, a high school teacher, and I can tell you at that time our schools were well-funded, our buildings were well-maintained. There was money for sports teams and extracurriculars. There was, and for special ed, there was every child had a textbook for every subject that they took. And then in the early 2000s, when my kids were in school, the government of the day started making cuts to schools and I joined the Toronto Parrot Network to fight those cuts. In 1995, the government took control of our education taxes in Toronto and since then, in almost every year, they've handed the Toronto District School Board a funding shortfall. This year, the funding shortfall is $28 million and the TDSB trustees are being asked to make drastic cuts to staff programs and services in order to balance the books. But more important than that, there's a 239 million ongoing funding shortfall that for programs that this government is simply not funding and this includes special education, it includes money for textbooks, it includes money for sports and extracurriculars and now the TDSB is considering cutting seniors' daytime programs. They're considering cutting grade six outdoor education trips and more. This is absolutely reprehensible to be making cuts to our schools, particularly for this generation of students who have survived through the pandemic and need more supports, not less. So I'm calling upon the government today to reinstate the funding for the Toronto District School Board and for every school board across this province so that our students do not face another round of cuts. Thank you very much. The member for Scarborough Center. Thank you, Mr. Speaker. I'd like to applause the Scarborough Walk of Fame, which has been around for over 20 years. This organization promote community togetherness and regional distinctiveness by commemorating Scarborough's many well-accomplished icons. The Walk of Fame celebrates Scarborough's rich culture, Mosaic, and inspire future generations by revealing Scarborough's native in the deserved domain of art and culture, community, education, environment, entertainment, fitness, health and science, and sports. Additionally, it stimulates economic activity to visitors in Scarborough and surrounding area, contributing to Ontario's reputation as a vibrant and inclusive province. The Scarborough Walk of Fame enhance the province's culture diversely as a cultural landmark. I would like to thank the chair of the committee, Mr. Glendebeermaker, his colleagues, sponsors, and a strong team of volunteers on the accelerating exhibition of Scarborough Walk of Fame 2024. It was wonderful to be there, amongst my colleague MPPs and other dignitaries who has seen the showcase of the inductees yesterday. I want to thank you, Mr. Speaker, for the opportunity to bring this message. Thank you very much. Member Statements, the member for Guelph. Speaker, Guelph's efforts to address homelessness shows what a caring community we are. Shortly after I was elected in 2018, I met with Dominica McPherson, director of the Guelph Wellington Task Force for poverty elimination, to strategize how we could implement their vision to end homelessness in Guelph. We started working to bring people together, and I'm proud of the way that all three levels of government, city and county staff, social service agencies, private developers, healthcare leaders, community funders, and citizens have worked tirelessly to successfully build three permanent supportive housing projects in five years. The community's efforts culminated with the announcement of operational funding for supportive housing in last month's provincial budget. Securing first capital and then healthcare funding for supportive housing have been top priorities during my time here at Queens Park. We have a long way to go to end homelessness, but I want to celebrate the progress we've made by celebrating those people who have got us here. Sheila Markle, Dara Allen-Ebren, and Lisa Burley from Kendall Community. Melissa Kowalski and Rachelle Devereaux, Guelph CHC. Kristen Kerr, Stonehenge, Gail Hoekstra, Stepping Stone, Kristen Kearney, Wyndham House, Helen Fishburne, CMHA, Emmie Perkins, Guelph OHT, Mark Walton, Guelph General Hospital, Jason Ashton, Skyline, Glen Abanda, United Way, Chris Willard, Guelph Community Foundation, Luisa Artuso, Wellington County, Shakiba Cheyani, and Michael Keegan, Guelph Chamber, Mayor Cam Guthrie, MP Lloyd Longfield, and Dominique McPherson, and many others in our community speaker. Thank you very much. Member Statements, the member for Richmond Hill. Thank you, Mr. Speaker. Today I rise to highlight a crucial initiative that we organize to support the community in understanding the three levels of government in Canada. Richmond Hill is home to a growing number of immigrants who may not have fully comprehend intricacies of our political landscape as well as the system. We usually do not meet in person, but this time we have it instead of a virtual meeting, we have an in-person meeting so that we can facilitate the communications between the speakers and the attendants. Recognizing the challenge, I'm proud to have the April Monday matters on April 22nd. This is a non-partisan and educational initiative designed to empower our residents with the knowledge they need to engage effectively in our democracy. This initiative will provide a platform for the constituents to learn about the three levels of government and understand the roles and responsibilities. We're honored to have the former politicians, including former parliamentary secretary and MP for Willowdale, Mr. C.S. Leung, former minister and MPP, Mr. Chris Kilgris, and former mayor of Wichita Stovill and chairman of CEO at Ryok Region, Mr. Wayne Emerson to share the insights. We trust that residents in Richmond Hill will benefit effectively, participate in this democratic process. Thank you. Thank you very much. Before I recognize the next member, I'm going to ask the members to produce the volume of their conversations, please. Thank you. Member Statements, the member for Perth Wellings. Thank you, Speaker, for calling the House to order for me this morning. It's wonderful to rise to talk about some important investments that our government is making through our recent provincial budget across Ontario, Speaker. Whether it's the 1.8 billion for housing enabling infrastructure, critical infrastructure to get more homes built across our province. Whether it's the 1.2 billion in the Building Faster Fund, 200 million for recreational facilities, Speaker, over the next 10 years, $15 billion to build new school, Speaker, doubling the amount of funding for capital this year, Speaker, and our provincial budget for our schools. And of course, $50 billion over the next 10 years for hospitals across this province, Speaker, from Toronto to Windsor to the north and to an Ottawa, Speaker. We're investing in Ontario, we're investing in the people in Ontario. I know it was important to see the $50 million for stabilization of healthcare capacity in our northern rural communities. It was also great to hear that we're gonna make the clinical extra program permanent, Speaker. I know this is very important to our rural hospitals, Speaker. Speaker, it was also great to see our government continue to build on our investments in primary care. Historic investments, Speaker. Over 500 million will be invested to expand primary care across Ontario to ensure more people can get care closer to home, Speaker. Speaker, unfortunately, all the members of the opposition voted against the provincial government, Speaker. They voted against primary care expansion. They voted against victim quick response program, Speaker. It is shameful. We will continue to stand with the people of Ontario. Thank you very much. That concludes our members' statements for this morning.


Very, very big round of applause for the people who are controlling the music up there.  Nime wa ona, very, very good job, since it's a quince Wednesday, we appreciate you also. Na students kumoja Brenda kwe WCW man say, sitawaza, ama fom, fom, yaa, I tried for Facebook, I tried for channel, on Twitter, hashtag is white and monika ibunisana studio. My name is Valentine or at color me val, ama val du kenileksana nomen yona in these hair streets. So you know it's about that time it's WCW crushing on our females and we have important things to discuss and today we're talking about dealing with pretenders. Weh, I can't wait for your comments, na jatustakwa too late, but in the meantime let us introduce our very, very, able panelists. How are you, Ni? Hi. How are you? What's your good name? Although, umu kwa kwa before, nuna kwa pwa ama uni toa pizwa, even in able to do like this so that they know you have me. Just, yaa, atu kiyongia today, yaa, uku e tuu kutu. Eh, you know. At least you are not taken, not engaged. Sasa, weh weh, but la kufokas on what you should be maintaining. Umu nangali apete. What's your good name? Uh, Praise Kende. Menda wapu, kwa apetu no kumili. Niki katushile kumalizia. How's that going? Amalizia iwi kariboni? April. Very soon, we can't wait. Praise Kende. On Instagram, Praise underscore underscore Kende. On Facebook, Praise Kende. And on Twitter, Praise Kende. Alright. Hi. Hi. You are new to our panel. You look very nice. Thank you. What is your name? Chayan Teji. Where where? Chayan Teji. Okay, for the sake of just shortening things, what would you like us to call you? Teji is okay. Teji is fine. Yeah. Where are you from? What side of Africa? That name is very exotic. Ha, western. We live here too. We cannot hide it from you otherwise. But where can we find you on social media? Instagram, underscore spicy dot 254. Where where? You even come with swag at a spicy. Hey, alright. Okay. Where else? That's it. Karibusana. Thank you. How are you? Yeah, I feel very, very nice, a beautiful lady says. Yes, yes, yes. To say enjoy too. Okay. Karibukosa. Wana kuitana niwe? Naitua Seriam Blaku. Social media sites you can find in Seriam Maestro Munda. All platforms. Alright. So should we just get, what do you think of pretend? Who is a pretender to you? Perhaps. Pretender is somebody who, okay, you present yourself to be something you're not in whichever way, maybe in person, character. Oja is straight surely. What do you think of pretend?  Someone who tries to put a different front or something different from who they are for a specific goal or a certain aim. Akonani ya? Yeah. They are gender. Xavier, I want to ask you a different question. Do you think I understand, I don't know if it's biology, am I just some type of science, mi mi we na relate na wewe, si we enta relate na mitu kama kaisu tu seme. Yes, you're both my friends and I know you from work, but mi mi na eto na nga uge yasi when you meet uncleyeshakae. So is that pretending? No I don't think that's pretending, it's the way you associate with both of us. So it's the personal and it's the way I'm personalised and I pay the price who I need to pay but I'm too different to you, you cannot always do the same. So what really is pretending? To the ladies I always feel it's one abyss, to the guy with the hypocrite. So basically, that's the one one. 1 upiwa na pretend? Yes, 10-to-10, but 2 me na wasi. Because women on kujang daily the guiltiness. Oku ima sensei diya wa kwa fana kwa kwa wana kwa very guilty. Nyi, nye maminga haya gareya lafumu na na kujakutu pedelek around Io lap, moja, mukise ma ni yeno. Ya, nene o the heart on ikihana. Ya, fe kata mita kwa umbeya. Igo your garekwa. I just wanted to win your heart. Mita wana lady, she's able to continue continue to continue. Please don't hold it in No, please tell him why So why should you hire a girl to please a woman It's something that's not yours like you're lying from the first day I'm not even going to trust you You see, first of all if I wanted to impress her even to get her contacts even to take her somewhere to say you connected me to her first of all I want to please her I want to please her I want to treat her well You see, and then you are being my friend you will be honest with me and say I want to please her I want to please her So I want to please her I want to please her I really have to go as per So it's men do that just in place but not for the long term That sounds like a very tiring life but I know also of some people who pretend that they don't know but they themselves are upside down Have you ever heard of such an instance? In church I want to say church loosely because it depends on me but when I see them they are holy they are holy that is why I am here I want to please her I want to please her I want to please her I know of a story There is this lady she is so churchy she has been to a church So all along she wants somebody who is God fearing and she wants to live a life but when you meet because when she meets people all of them pretend to be what they are not what she wants So at the end of the day the true colors are together Which is true So you are on pretenders A lot of retailers on the religion side because your parents tell you that when you want to look for a good wife there are two places of getting a good wife either at work or in church So you see a lot of men going to church to look for women So you see a church where you can see all these avenues but she is not getting a right person So you can see a church because church you view it as a very holy place So you are going to get a very holy girlfriend to live with her So you can see a lot of men going to church and you can see a lot of women going to church But now there is a problem because men nowadays mostly like most of them go to church to get a wife material So when you see a church ladies that want to go to church to pretend so that somebody will also get a wife So we are pretending Niliyambuwa kani sanika hospitali the people inside some of them are still sick some of them are undergoing healing sihati utapata kanyo naitisha just be careful ok So here we have the first slide pretend the definition So it's an attempt to make something that is not the case appear true So something an attempt to make something that is not the case appear to rule that is what pretend is Ayasusa vinyuwa stanna tunajua pretend What is one way we know how How is one way we know how to pretend Why ladies pretend in all ways always So one I'll entangela kitu jeneru I'll entangela kitu jeneru Kitu jeneru I'll entangela kitu jeneru I'll entangela kitu jeneru kia and life in parcel Like people really pretend on Instagram kwa I mean it made me dangerous Onanda kupos kwa gariya wene I love wana sana Take me back Many people are always telling us wele ni goals, work hard Bible verses then Okiru kuhuma the story is completely different How do you think we pretend I think some ladies like in real life they are ratchet but when they're with the guy or someone they're interested in wana kwa pole and sweet kini tunata kuskia that's what you get At the south view, but it is Oh my gosh, babe How have you witnessed I witnessed what stanna kii pretend and it had nothing to do with you lakini wona wu stanna niya me tu pima wu yuehe Funny thing, men are really good to to know if a lady is pretending Hi If you are so good, that is a lie Men are really good Excuse me? No, excuse me This is why Kitambu ni kwa na shanga mtu wana semati Oh, he stole my man nama kitukayo And then they came and told me ok, men are a little bit weak So them tu akimuguzatu mahalifu lani anezamu nipaswe you cannot tell if a woman is pretending Please allow Just kubali to a delen na meisha Tu kuna kamaati And every after the date you will bring the report to the kamaati Squad And they will accept ah, uledema kusawa uledema kusawa lakini Kuna zingira tu chochu zingina na Funa lakini She is really pretending There is relief versus reality Those people pretend to to impress others But on the reality it is very open You cannot match those standards you are trying to pretend to be So how can you tell if which happens to be a next slide Can you tell if someone is pretending and how? First of all if you are not high class it can be any and cannot You are pretending to be high class but you are not high class Ah, jih First of all if you are in a poor situation and you cannot come and hear you are pretending Excuse me, I thought that if you were in a poor situation you would have never come and you are in a poor situation Me, I am a young woman I think that if you are in a poor situation you will be in a poor situation I always just keep quiet I don't know if you are in a poor situation but it is not the end of the day The way they dress I don't know some clothes don't match you What does that mean? I don't know how I can... Is there an example here on this set when a sissy takes out that one and a sissy does it because I am the one who does it No, she is very professional at this moment I don't remember if I am in a match and I am the one who does it Don't pay a spot light Don't pay a spot light Stop working as a spot light No, Fuuatura I mean these are goes to the people I hang out with them I don't hang out with them a lot apart from work so I can't really tell it's close really much with you but for now you are really beautiful you look fine You made your call because I had you Can you tell if a girl is pretending that maybe to some you just met them and they are not going to behave as in Gimali Can you tell if they are pretending? I think you can like according to how she acts now and other people like maybe waitresses and what you took as a treat kwa ko ata pretend but to other people when she is not trying to get anything from them hata kwa na yote mi aku difanya sana That's the difference So she will be nicer to the person who has something that she wants as opposed to How do you think you can tell a pretend if she has an accent but she has a passport I think you can easily tell when someone is pretending unless if that person is really a good pretender like a professional pretender otherwise you can tell when someone is pretending I don't know how I feel because no one can tell when you meet if you are pretending I think for me I think you can easily tell when someone is pretending kwa pesa Mr. Yana, don't say if you don't admit she really shows some concern that you are supposed to sell but at the moment it's like a little budget it's like a little budget it's like a little budget it's like a little budget it's like a little budget it's like a little budget that is a whole scheme from experience you need to come when you are in pitchment immediately can we please have our next slide because I will be giving a couple of scenarios this is a fact first and then a couple of scenarios so though most aged to admitted ladies judge each other on looks age and sex appeal please correct me if I'm wrong wasdana we judge each other by looks age and sex appeal my wrong and if I'm wrong why no I think you're right how does it make you feel entering a room when you go to a room but you model and go to a room it will affect how you feel how will the modeling one and this other one affect you so I think like when you judge women judge other ladies according to how they look how they dress in the age what you want to do because they think I can sleep and here ever since I got this hair color my friend reaction by this was very fascinated wow wasdana wengine wengine wasdana wu wengine wengine it's the same face just different colored hair I don't know why there is a problem how do you relate if perhaps maybe in a place who has rainbow yes when in rainbow but there is just a certain feeling wu kusha nga piliyoryYa piliyoryYa high ccityziu rainbow Because, for example, okingia place probabili kuna, like people say on a model, you know how willewako, maybe dressed, make up and all that.  So it's, it's feeling poor. I think that is why it's very important to have high self esteem. Dokabu loko tena otwing, achan kwen bihata story, vee vee life story, juzit me kwa pameru university, they're having amista enumis. So send li kwa backstage, na mimi me va tisha tia wa itu fefu, na jeans, na life imende. Latas kwa na make up pa isi wei, kwa ni kwa kat. And then all around me, beautiful people and beautiful things, very different sizes, tall, a little bit like that. I even saw there was a plus size type situation for the models. And it, I would have felt bad kama singe jiju wa aki wa lai, kwa singe jiju wa nge jibu kiva. Ona, sasa, wuna make up ni sawa, uko job, sawa.  Focus. A lafu sasa wengine sa I can now celebrate you for being beautiful. But lapse came by. Can we do that? Is that something we can campaign for girls? Yes. So kuna shida mahali. Not siwa s'chana wengi wa rafanya iwa. Not for real. But it's so, if your heart feels nice when you do that. The problem is, most of them hawa jaji exit. Like kama hawa jaji kubali ningu mosa na kukupne situation, somebody else out there. That is why you'll see very many people shaming others online because of things like that. Why are you laughing? Why would you shave your fellow manomestli ataka ma? Ni ni may happen. I don't see. We all know everybody wants to outstand and outshine. So basically every lady will always want to outshine the stage. But at the same time, I always wonder, wana mademo wa super, wana tendu kwa appreciate madem sii wile wa super. And all the madem when you say wa super, they don't like, but ladies were very beautiful. I don't know why. Kuna wone zava na patem mtu anani beke atu attitude for no reason. Na ni mstana. Na na stakujana, bada stakujana accent. Uga kusungu mingi. But the way she's treating me, ki doga tani nivai nijifiche kwanza. Okay, do you want me to look bad so that you talk to me? Like, what's the problem? Have you had the experience? Yani mtu tu atu uga ungeya. You've not even presented yourself yet. You've just walked up to them attitude. For? I think ladies, some ladies feel threatened. But we cannot be beautiful like you at the same time. Yes. It's so imagine. Like, onna viet ma kaivi kwa. Kilam taka na utimbake. See, vieta na zata nga nyikiwa pa say. No one is feeling jealousy of anyone else. Ha! It's okay. Next slide please. Remember you can give us your two cents at Y245 on Facebook at Y254Channel on Twitter. Hashtag is Y in the morning. So, what can you tell your slide here next? Uhu. Do it question time. So how would you relate to the following? Then we immediately go to the next one. How would you relate to the following case scenarios? I have. I have the ones who pretend to be fragile. Shepata hastana. They cry in their emotional and they just blackmail it. So, for example, tkewa iwi watatu. Yani yongongo ya she's ratchet like illet. Ushai ona hastana ona sunda. Boflo easy ndo wa kule bisuri. Pa tichalia kikam. Oh my gosh! I don't even know I'm going to get home. I'm going to pay for my Uber because. How do you do such a client? It's difficult.  At Tomsavia. Ntumetokana ea apashama hohotu kichira ka bezu. Sa, ea ata hoji ea ziku nyuaish. Can only take from mind glass. What's the problem? Simi na kuhetitu na reality. Ah, ya. If you're not like this and you're presenting, I'll just let you know. Sasi ya mebebo na crowd. For example, if there are like three more savias and she's all up.  Awa ta kuwa. Oh mama. Sa sapa uta anza. In fact, uta kaita ukenza kongef. No, na kutu. I think da konga liya tu na. I'm done with you for real because. Nipu akua real. I think that's why you always see men really taken advantage of such characters. They always use such characters for men. Baba na de. How do you feel? That's why you don't know me. Oh so you know. Me na ne maga ubo tila wa katu. We will go to ta nipa yo. We'll pay. Touche nipa ma rambili na. Ha ha. But the moment you're done with you, ta kuna text, ya lenda za kudu na nga hubi. Mwabi. Miwa ya ning. We cut off the ones we've already used. Ikun da niya wanaume. Kwa so watu na feel ba ya. Where we reached, ta kwa ki na peyan baya wako. Anisha na me peya profile ya kote e? Nakudyu waka te? Yaku tende. only a few weeks ago was never out of our house to hold a game we pleaded to design your for us so you did it so I will go with you but I already know in my plans I am pretending what are your hobbies? bungee jumping what is your dream? my dream is a little more you say her name is Padamata Faww your friends give you a name I told them I am a padamata I am a winner I am doing this How would you deal with such a person? I can't pretend, I can't pretend. You just be a hater, it's okay. When the other men think you're hating on her, it's okay. It's just not right. I have a story. Kuna umstana fulani, mungu amu sedi.  Kaunani skia, please get some help. Umstana lini kusia. I laugh, this is Val minding her own business as usual. Minding business. Aka kuja kuangu. Malili kuwani meka. Akan tafta. Vzuri. Aka ni explain ezo vitu zote amefanya. Vini amenitenda. Vini e. Atas ehi. Yani ezo vitu ali kwanani yambia. I was like, ehi. Yani you're just telling me, to my face, that's what's happening right now. How do you just, you don't even have a reaction. You can't even be angry. You can't even be upset. There's no for exploding. Uuna relax tuu naskiza. So this is what has been going on. Aya. So after that, I took the necessary measures.  Kamsa. Aya. The next time tunapatana, ili kuwatu batinbaya, e streets ane robi. So nukamu ambia. Ona, since, I still come and you listen to me. I laugh. Ona. Sikai ili wukumeni ambia before. Oh my God. I just say for you to come here. I'm like, okay. I'm telling people. Oh my God. It's such a lie there. Ehi, ehi.  Mentally ill. Uneza jini tenda. Ukujo ni ambia. Alafu kana tenda. What is the problem? How do you deal with someone like that? See it's just for prayers. Prayers and cut you off completely. I will give you a drop kick. If you come anywhere near my physical area. Are we together? How do you deal with someone like that? Nak. For real. Like for real ako. Oh my gosh. Ba. Ni. Sikai ili wukumeni ambia. Did you forget? Did you hit yourself? Like why are you in an accident? I'm an easier. What is the problem? Vitu ni bili. Eda ni gondroa. I'm a jinga. What is the problem? How do you deal with that one? Actually both. Talk to me, sweetheart. It's perplexing. So, I can talk to you. Now, I insist if you want us to get physical, we can. Ba, let's beto it's not the answer, guys. Laki ni uchinga zingine pepeki ala ni. So, kai na mamama ako. I saw something, I'm paying here. Remember I tried 254 on Facebook. I tried 254 channel on Twitter. Hashtag is why in the morning. I have another scenario for you. But before that, let's start with the comments. I have 19. Good morning. Good morning. So, you opened your mind a little. Ok, one now. Chawa wumandani kwandani. Jihadani, not your money. We only live once. Ok, for those of you who don't understand and you're watching us on DSTV channel 276. He just said there are people who don't like it when you prosper. Ba, good morning. Good morning, pa. Double or one. Mambasat kondani as always. Jay Oswally ni a queen. So, we not say or add anything. Melody says good morning, guys. Good morning, kitty. Maybe, ok, we'll show how you have progressed in your life and you see the first expression you will be able to see if they really want what's best for you or not too.  Kungoni. They are called kungoni. Namba 3.  That's how they don't want you to succeed in life. Wao. We have Neema Wambogo. She says watching from Nyeri. The one thing, the one you think he or she is your best friend. He or she is the great enemy in your life. Never open your heart for someone because most of them are the ones who think negative about you. Wao. Ok, let us start with kitty melodies number one. Hi. When you tell someone you've progressed in your life and their first expression.  You know what? No, it's not coming. It's not coming. So how, and they were your friend. How do you move on from there? And I don't know what's done and I don't know how to sumbo because what's done is said when they do how to sumbo via kili. So it's usually someone that we've called friend. Someone who's close to us. How do you deal with that one?  So sumo misa kii kama hako takii mazyu rishueli. E tuwa chetna yos kuli. There are more friends in this life. In fact, at our standard kawengi kuli kwa nome. You'll make more friends. How would you deal with that? I think, because you're ready my friend, obviously, kuna vilechul kwa tuna saideana in some way. So I won't cut you off, but I already know like your intentions. So I want to cut poli poli but I want to convey what I share what I don't hear. I like that because umo jo ni had it wishi. There are some cases you should just remove. Kabisa toka. Leave it. But umba kata wishi we cannot alienate everyone. So just be careful what you say now. Just be careful. Umpe wongo. Wone malista kika. Experiment na ni. Sebe, what do you think about this conversation? I think you can use your innocence and try to assume jo utajende, and then wait for her to come and give you buddha and appreciate her. So just be smart and come jig. Kuna... Oh, okay. Can we have the next slide please? There's not the next scenario which is making me a little bit happy. Okay, not happy but it's the thought. All right, so we have the ones who act tough and usually have a lot of aggression in their timina. As in, but inside, very, very small. Very, very small. Adopt kanaizoma to sizote. Oh! Weba toji mi nani. Nya, nya, nya, nya. Nya, nya, nya, nya. Nya, nya, nya, nya, nya. Nya, nya, nya, nya, nya, nya, nya. Nya, nya, nya, nya, nya, nya, nya, nya, nya, nya. Depression. Oh!  How do we help those ones? Ya, nona ni sawa kwenbe kenye anatkak kwenbe ya wewe. Lakin ni wewe umgoze tu. We should let them know that vilewa wana kuguze evo. As in, kama wakona isu na uki respond the same with aided. You should let them know how it feels na respond evo nakizke weba umo ujerebu kumone. Sure, but that is how you make me feel too. Is there a way we can just use words instead of kudungana? A knife for an eye? Is there a way we can just sit and talk? Kama some people cannot just be talked to. If somebody you can sit down we can talk, that's okay. But if somebody that cannot be talked to then... Say, we won't know naji. Kablami fiki. If your friendship is really based with Zuri which is very hard to approach someone who will explain it. So I think to develop to relate to the trust that you develop you can say maze achaku jisukiya. Maze achaku preten. Which is very hard to kumbia muntu. You will spark another conversation. So I think if you can able to develop the less kids you can approach muntu that's why if friendship should be really based well. Kama iku based power una mombi atwe achaku nifana evi na evi. Wei ituna enda evi. Iyo for me. Wei ituna enda evi. But you see for ladies I can't tag along with you guys if you are going there.  But for the guys atwe to enda evi. But you see for the ladies you see. Ladies should also learn muntu kwe li. First umse mambia evi na evi na evi. How do you base a friendship properly manze evo? Una juaje is different iku kwa simiti not on sand. Iku kwa solid. Iku kwa friendship mimi kwangu ikama muli sumana mse for that while me jwa na juuku kwa kuhu sumana mse iskulu ma primer muka metiseka. Muka kwa raha. Muntu kwa ezi kwa na kulingia na ulu kwa na mijiwa hapum belemi kama kama it's high school based kama the schooling based kama if it's work apuni na kwa nga mbaju kazi wato me patanatu. Uju muntu wema liishi. If you guys come from the same place at home friendship can be based apu kama muli suma puma je it can be based apu kama you guys just met under some funny circumstances na muka jail, muka associate it can be based from there. Can I just use his example to ask your question. Pahaps me biniwote me toka place modus you at same location or area. So it just so happens that you've known each other for a couple of years. One of you does better than the other. Nasi and again I want you to understand it better than kwa gani quotes because it may be my season maybe it's my season or it's your season and it's not mine. But excited as we are to meet we don't have fast reaction so how do we deal with that? If you are the one pahaps maybe who was left a little bit behind tawana mwenzako ama fallu na she's going to do for whole day. I think I'm going to support her If she's a good friend, I'll obviously benefit from it.  Very, very smart. Explain benefit. No, if I was her friend that had done better, nani kwa dubai, mwa nani similete vi tu kava? Mwa mwa mwa mwa mwa mwa mwa nani dubai nani. In fact, why not? Okay, apu kwa dubai. It depends where I'm going with. Mwa mwa mwa mwa mwa mwa mwa mwa mwa dubai. I love to watch your Kenyans. This is what I want to do. I don't do Kenyans. I'm only doing dubai. Ideas, girls. Maybe I'm a serious person. Okay, the next scenario. The ones who pretend to be your friend only to pull you down when they think you're getting better at them at life. Actually, I don't know what to say. And it's it key to you, Mizamu, too. Because when they were your friend, maybe you were at path. You were doing things. Akiwana idea unamrushia.  But suddenly, kangu kame go through mahali manze. Maybe at any kwa na kushikam kona when they see water, but where piasa, niki kushikam kona niku inuawe unanini ni. So how do you deal with that? Okay, actually from experience, I've had a friend she's from Tanzania. So I knew her through another friend, a friend of mine in Kenya. So we became friends, like the three of us. Lafu vitu tunafanya zina. Ziko grounded as in Pomodzenik where environmental ambassadors were always plotting trees together like I do videography. She sings so tunafanya. Wow. So now, I decided also to help her shoot videos which she has not done before. So I decided also to help her shoot videos which she has not done before. But then, she goes to this other friend of ours tells her bad things about me and then comes to me, tells me very bad things about her. But then, this friend of mine doesn't know that nimi ambuizi vitu na Sripiaia miyandiyo. So like kia na kagi jizambona ui unanimbevi tunbaya kuliko praise mbona na mina juliza kumeksiju. But then there's something that she said that had us confront each other and she said to me, nimi nambia kumesema, nambia kumesema. So when we confronted her, she was like, I'm the victim. We know you. We know your handwriting. I said, oh, I blame her. I don't care what she says. She clearly told me that na najuwa na najuwa ni nambia. But then she's there all over. She's the victim. Social media posting everywhere. So she just cut them off completely. How would you handle that? Agree with her. Just cut them off. They know how to cry. I don't see why I really want to go anywhere with somebody. Because at the end of the day if my friend and I did not like atukua wajansi, we were like kningishi kumbebaiva kumasa do something to her because atukua wajansi na najuwa na najuwa na najuwa na najuwa na najuwa na najuwa na najuwa na najuwa na najuwa na najuwa na najuwa So I don't see why I blame somebody like this. I don't get the point of that. I don't get the point of that. If you don't want to be my friend and her friend at the same time, just let us know. You can be the victim of me. It's okay. It's okay. And what runs through your mind when you do such things? I don't see why I blame somebody. But I think it's really okay to be jealous. It's okay to be jealous but also try to come out of it because if your friend is benefitting and has an opportunity, maybe he's going to open doors for you. Maybe God will give you two ways of talking and enjoying him. So it's very okay to be jealous but it's also good to pretend sometimes. Sometimes when you pretend, it's beneficial. Pretending how? Ya, you see, if I always pretend misi na kazi, misi na nini, na teseka, someone is able to see that baby like cry from my side, na kani sa idea.  Other for the ladies, kia za kupretendivo, kujieka high class. Ako leti kua attract watu high class. Na kula wanana, na kumina, na kwangatua me potia. Potia wata kuchukuatuivo kwa hende le kuku pandish. Kuna wale bright minds kama sisaka. Ta kukanyagi atu kia kote, urudi sa sa ching. Ki what? I don't know if I agree with those sentiments. And this is a truth to na tumi angusha pavitu. Na wepe kia kundu jangusha. Kukaribu kwangusha story. So kuna umtu. Misha na atu, we're friends again. Mimi iniki pata rafiki to seme, sana sana was sana. I really like to share ideas. I'd really like to see ladies getting that money. Mina pwenda sana nikiyo na dey mame akondani agari kubakubazen. I want all of us to go there. Me hasot, me hasot, me hasot. Aki dop doguevi. Nika pata kitu maybe a little bit higher than her. Sasa this is where the amazement comes in. So to seme, maybe wame ni umgezea pesa yu placingi nesindo. Sasa ananzakuni tisha pesa because now you believe. So now unani pangia, ya angu. Nia tia tiwa ume ako because I know also you're her thing. So pesa zako mi zako. What is that? Saitan. No sense. Hashtag when the morning. How do you deal with that? Atimi alini amaze. By the way, alini amaze. Nali jam hadia kanzaku wambia watu wene mi nm Stingi. Excuse me. Are you not? Na oni mtotani yambia ako na machali watu faniya vi. I'm good for you. I feel like my intestines are aski aka zona. I don't want to do that to myself. For men, how to trap their fellow men. If you're a search character, make sure to ume mwamba na taku zami how much you want to take. Na kumia ok na kupia alone. So siya taju aki kupia alone, it's going to be difficult for you to pay jumezoa nana yura fukien. So the next time unata kukuzea, unaji jaze tu e by the umse ni kwa mi mwamba alone. Na kumia ok na jaze ni pado. Anakutu ako hiwa story bi basala. Anakupia hiwa alone nana taku. Then it's going to be difficult for you to come for the second time. So you can always trap this guy by oh nata kwa mancha shika. Ata kumia kikuzea ma rapili so nami jibutu wujane wujane lipa. Actually me do that for the lady. Mi wuku sa idea pesa. Na jibutu, then a second time unakuzea. I'm very confident. Ile wunana what's up, nana krua pili na wujane lipa ido bad. I thought to agree kini lipa nana kwa ungeza. Ndotuna. Aki jibutu, akia I'm standing and I'm going to say ok you just work on paying my loan and then I'll sort you out. Na oni watu wana kukuzea. Sija punyima, we are very okay. Haatun doa ata kupigia 10 times kuitisha. Ata kani punch. Lakini kuru deisha. Umpigia 5 times. Panch doi taku fanyu pigia evi maramingi. Uwani nani sumbo. I thought you needed it urgently. Now that it's me asking for it. It's me asking for it. But disrespect is okay. I hear we have Facebook comments. Please keep them coming. We have Nikola Sabastan. Says good morning Vihiga finance boy all the way from U.S. of Shiro. Mosina Tazama. Kaldinam Super says the way they react when you tell them like for instance ok and bear your good news. Mtu nona that good news is not so good to them. Eliza Steve says I will never introduce my mind to so called friends. Good morning from 18. Wanansi says watching from Tekaisi. Wanansi holy kapa lot watching from Kapsapet. Again Wanansi says always watching and good morning. So apart to mejuan. When you to nambia good news na wanakayo good news nikahimia omiza roho kidogo. Maybe I want to ask and this slide li kwa kuku conclude because I said to kianza kuwana vitu zawingine piatwana zato sindio. So that means at one point mimi personali mimi kama falantai na jo nisha ipretend. Maybe it was to make myself feel better in a place maybe nikwana feel I am not enough of whatever reason I was pretending. So how do we stay real? I think for me the people you associate yourself with if you guys are associated now a lot wana juwan. So just associating your kakuni na juwana na muntu and trying to improve others keeping the smile, being happy all the time it helps you to not to pretend kaw ko broke mimi ko broke. kaw ko na pesa mimi ko na pesa to learn to jibab kai kukidogo na kukidogo na kibuku isha kisha na kujia. So being real at the same time saying the truth all the time wana juwana uta pretend. But I also wanted to ask a question do parents pretend? How? What do you mean? In what context? Financially do they pretend? I don't think it's really pretending maybe because we said pretends is trying to make something appear real that is not. But I would assume me niki lelewa the times that we didn't have so much kaw ko na kalisha nga wana pesa mimi isha relax. Tu na tiza tu kasi si maratu na kulaugali na skuma like 5 times na wik na witi si nga maju na na tu the look on people's faces na na tiza tu chini but you my parents I knew had my best interest at heart. So at akaon na nifichia vitu sivi tu sta kujaku ni umi za mimi. What about kama mama ko na kumbe nivi le tu atasima na pesa jatagi kuna kama mimi kwa mama hali it is a myth african parents always have money sana fathers. How would you think parents pretend? At times. Ki aje. In very many ways. Okay. Perhaps. Sorry. Let us just conclude. How do we stay real? By loving yourself.  Kuna siku tu likot nongelia stori flani apa I can't know what county she came from and it's not important. Ali toka county flani mashambani a kakuja nae robi. I don't know what kind of peer pressure hit her. Akainda kwa duka akaibawig akaengizua kojinia kengizua jela. And then okay it has a happy ending because it turns out what to continue from home and then you come here it's like you're not a lady if you don't have a wig. So choose your friends carefully. Nasi wakwe katu post I'll be with you shortly. How do we stay real? I think we stay real by being honest accepting who we are and being okay with who we are and also seeing the kind of people you associate with because you are not a peer pressure in different ways.  So maybe you'd have started out not a pretender but because of the friends you have suddenly started pretending. For example when you have people that are always going clubbing to high places you're their friend you need to be there maybe probably and you cannot really afford that. So maybe you really have to probably when you go there you have to pretend that you're not first sayo yaku la the whole week so you need to stay with your friends. Oh no we are jekers. Stop laughing at your friends. I see those things a lot of times. But also when it comes to standards as you want to maintain your own standards ladies are very good even men are good to pretend on the higher standards but also let us learn to pretend also on the lower sides. The lower group na coldness they adapt flexible. It's very difficult to give advice on things that are ongoing. We're always learning and I'm probably going to have a chance to pretend. But I like to believe balance niki to poor in life so there's contentment and ambition be content with what you have and who you are but be ambitious enough to want more and get it the right way. I'm not getting my friends. That's why 254 on Facebook and 254 on Twitter. Hashtag is what in the morning Love you very much and thank you for staying with us the entire morning. We have a repeat today from 2 to 4 and weekend I can see you from a distance. I can't wait to meet you once again. Have a wonderful day and the rest of your week. Bye.


Welcome to this ministry update for Iglesia Biblica Antorcha or Cornerstone Guatemala. Today I'd like to be able to encourage you by informing you about all the different changes personally that the Roosie family and the Mudge family are making and having in this time. We are preparing to be able to sell all of our things, leave our jobs, and move to Guatemala. So in the selling of our things, we're preparing our cars to be sold and we have had a church sale or a sale of all of our possessions at the church property. We are beginning now to look over all of our personal possessions and try and think through whether we're going to take that to Guatemala or not. We are resigning from our jobs or have resigned from my job and Lee has resigned from his job and those are big changes for us personally. Our wives are preparing the homes, they're preparing and packing and we now have a home in Guatemala that the Roosies have signed for. And we're excited to be able to complete all of these logistical things to be able to prepare us for Guatemala. One thing that is very impactful about looking through all your possessions and considering how life is a vapor. If you read in Psalm 49, in verse 10 it reads, For he sees wise men die, likewise the fool and the senseless person perish and leave their wealth to others. Their inner thought is that their houses will last forever. They're dwelling places to all generations. They call their lands after their own names. Nevertheless, man, though in honor, does not remain. He is like the beasts that perish.  Like sheep, they're laid in the grave. Death shall feed on them, the upright shall have dominion over them in the morning and their beauty shall be consumed in the grave far from their dwelling. But God will redeem my soul from the power of the grave, for he shall receive me. In Psalm 49 it teaches us about wisdom and foolishness.   We're gladly selling our things and laying them down for the cause of Christ because we want to have this kind of wisdom. We want to be able to gladly lay these things down so that we're thinking about eternity. It's the least that we can do in light of what Christ has done. So please pray for us as a family that we would gladly be able to deny ourselves and lay aside the things that we want so that Christ may be honored in the life to come. Thank you.