Srednicki Chapter 36
|
|
- Ἐλιακείμ Κοντόσταυλος
- 5 χρόνια πριν
- Προβολές:
Transcript
1 Srednicki Chapter 36 QFT Problems & Solutions A. George March 1, 13 Srednicki Using the results of problem.9, show that, for a rotation by an angle θ about the z axis, we have: DΛ = exp iθs 1 and that, for a boost by rapidity η in the z direction, we have DΛ = exp iηs 3 In problem.9, we showed this is true for the vector representation. It must therefore be true for all other representations, including this spinor representation. Srednicki 36.. Verify that equation is consistent with equation Equation is: Using equation 36.39: γ 5 = i I I σ1 σ 1 γ 5 = iγ γ 1 γ γ 3 σ σ σ3 σ 3 Doing the multiplication: σ1 γ 5 = i σ 1 σ σ 3 σ σ 3 This gives: Now recall that iσ 1 σ σ 3 = I. Then: which is equation σ1 σ γ 5 = i σ 3 σ 1 σ σ 3 γ 5 = I I 1
2 Srednicki a Prove the Fierz Identities χ 1σ µ χ χ 3σ µ χ 4 = χ 1χ 3χ χ 4 χ 1σ µ χ χ 3σ µ χ 4 = χ 1σ µ χ 4 χ 3σ µ χ Recall that the right-handed fields are always written as Hermitian Conjugates of left-handed fields. Thus, we insert the indices: χ 1σ µ χ χ 3σ µ χ 4 = χ 1ȧ σµȧa χ a χ 3ċ σċc µ χ c 4 This is index notation, so we can move these around as we like: χ 1σ µ χ χ 3σ µ χ 4 = σċc µ σ µȧa χ 1ȧ χ aχ 3ċ χc 4 Now we use equation 35.4: χ 1σ µ χ χ 3σ µ χ 4 = ε ac εȧċ χ 1ȧ χ aχ 3ċ χc 4 Now we use the Levi-Cevita symbol to raise the indices recall that the Levi-Cevita symbol is the spinor analog of the metric. We also move them around at will. Then: χ 1σ µ χ χ 3σ µ χ 4 = χ ċ 1 χ 3ċ χ a χ a 4 Now we drop the indices since this are just multiplied: χ 1σ µ χ χ 3σ µ χ 4 = χ 1χ 3 χ χ 4 Now we want to get back where we started with 4. We know that χ χ 4 = χ 4 χ. [If you re confused about why the fields seem to commute when fermions should obviously anticommute, see equation 35.5.] Then: χ 1σ µ χ χ 3σ µ χ 4 = χ 1χ 3 χ 4 χ This shows that the right hand side of equation is invariant under this relabeling. It follows that the left hand side of equation is also invariant under this relabeling which is exactly what equation claims. b Define the Dirac fields Ψ i = χi ξ i, Ψ C ξi i = χ i Use equations and to prove the Dirac Form of the Fierz identities, Ψ 1 γ µ P L Ψ Ψ 3 γ µ P L Ψ 4 = Ψ 1 P R Ψ C 3 Ψ C 4 P L Ψ
3 Ψ 1 γ µ P L Ψ Ψ 3 γ µ P L Ψ 4 = Ψ 1 γ µ P L Ψ 4 Ψ 3 γ µ P L Ψ All we actually have to do is prove that these forms of the Fierz Identities are equivalent to those in part a. Let s start with equation 36.58: χ 1σ µ χ χ 3σ µ χ 4 = χ 1χ 3χ χ 4 On both sides, let s write this as a bra times a ket. [ ] [ ] [ ξ 1, χ 1 σ µ ξ χ 3, χ 3 = ξ σ µ χ 1, χ 1 4 χ 3 ] [ χ 4, ξ χ 4 where in the last term we remember, as in part a, that χ χ 4 = χ 4 χ. We can use equation 36.6 to identify some of these terms: [ ] [ ] [ ] [ ] Ψ 1 σ µ Ψ χ 3 = Ψ σ µ χ 1 4 χ Ψ C χ 4 3 ] On the left-hand side, let s separate the σs into their own matrix: [ ] [ ] [ σ µ χ σµ χ4 Ψ 1 σ µ Ψ 3 = Ψ σ µ 1 χ 3 ] [ Ψ C 4 χ ] These are gamma matrices: [ ] [ Ψ 1 γ µ χ χ4 Ψ 3 γ µ ] [ = Ψ 1 χ 3 ] [ Ψ C 4 χ ] Now let s rewrite the remaining kets as projections: [ ] [ ] [ Ψ 1 γ µ χ χ4 ξ3 P L ξ Ψ 3 γ µ P L ξ = Ψ 1 P R 4 χ 3 ] [ Ψ C 4 P L χ ξ ] Using 36.6 again: [ Ψ1 γ µ P L Ψ ] [ Ψ3 γ µ P L Ψ 4 ] = [ Ψ1 P R Ψ C 3 ] [ Ψ C 4 P L Ψ ] which is To prove 36.6, let s go back to equation and write it as a bra times a ket as before, but this time we will write the last term differently: [ ] [ ] [ ξ 1, χ 1 σ µ ξ χ 3, χ ] [ 3 = ξ σ µ χ 1, χ ] 1 4 χ χ, ξ χ 4 3 The left-hand side has not changed; the right hand side is the same up to an arbitrary relabeling 4. We can therefore read off the result from equation : [ ] [ ] [ ] [ ] Ψ1 γ µ P L Ψ Ψ3 γ µ P L Ψ 4 = Ψ1 P R Ψ C 3 Ψ C P L Ψ 4 3
4 This shows that the right-hand side of equation is invariant under 4. It follows that the left-hand side must also be invariant under that transformation, ie that: [ Ψ1 γ µ P L Ψ ] [ Ψ3 γ µ P L Ψ 4 ] = [ Ψ1 γ µ P L Ψ 4 ] [ Ψ3 γ µ P L Ψ ] which is equation Note: This may seem like a brilliant but completely unintuitive solution. If so, just start with the result, apply the projection and gamma matrices, and arrive at Then reorder your results to get this solution or announce that all your steps are reversible, so you re already done. c By writing both sides out in terms of Weyl fields, show that Ψ 1 γ µ P R Ψ = Ψ C γ µ P L Ψ C 1 Ψ 1 P L Ψ = Ψ C P L Ψ C 1 Ψ 1 P R Ψ = Ψ C P R Ψ C 1 Writing both sides as instructed, we have: ξ 1, χ σ µ? 1 σ µ = χ ξ σ µ σ µ ξ ξ1 Doing the matrix multiplication: ξ 1 σ µ ξ? = ξ σ µ ξ 1 To see if this can be true, let s insert the indices. As usual, the daggers represent righthanded fields, the non-daggered fields are left handed that s our convention. We give dotted indices to right-handed fields, non-dotted indices to left-handed fields. Further, σ takes raised indices, σ takes lowered indices. Then: ξ a 1σ µ aȧ ξ ȧ? = ξ ȧ σµȧa ξ 1a On the left-hand side, let s use the Levi-Cevita symbol to raise our indices. Remember we have to contract with the second index of the Levi-Cevita symbol, otherwise we get a minus sign. Then, ε ab εȧḃξ 1b σ µ aȧ ξ? = ξ ḃ ȧ σµȧa ξ 1a Now let s use equaton which is a definition: ξ 1b σ µḃb ξ ḃ? = ξ ȧ σµȧa ξ 1a In order to be able to drop the indices on the left-hand side, we need to reverse the order of the two terms. However, note that the function indicated by the index of a Weyl Field is a fermionic function, and these always anticommute. Thus, ξ ḃσµḃb ξ 1b? = ξ ȧ σµȧa ξ 1a 4
5 Dropping the indices, we find: ξ σ µ ξ 1 = ξ σ µ ξ 1 Expanding the second equation, we have: ξ 1, χ χ 1? = χ ξ ξ 1 This gives: ξ 1 χ = χ ξ 1 The third equation is evaluated in the same manner as the second; the result is χ 1ξ = ξ χ 1 by is true see equation Srednicki Consider a field φ A x in an unspecified representation of the Lorentz Group, indexed by A, that obeys UΛ 1 φ A xuλ = LA B Λφ B Λ 1 x For an infinitesimal transformation: L B A 1 + δω = δ B A + i δω µνs µν B A a Following the procedure of section, show that the energy-momentum tensor is T µν = g µν L L µ φ A ν φ A The derivation in chapter still holds: everything is the same except that we ve replaced the scalar field φ a with the representation-independent field φ A. We therefore read off the energy-momentum tensor from equation.9; the result is equation b Show that the Noether current correpsoning to a Lorentz transformation is M µνρ = x ν T µρ x ρ T µν + B µνρ where Equation.7 gives the Noether Current: L B µνρ = i µ φ A Sνρ A B φ B j µ x = Lx µ φ A x δφ Ax K µ x
6 We need δφ A, which we get from the symmetry. Our Lorentz Symmetry is, in differential form: φ A LA B 1 + δωφ B x µ x ν δ ω µν We use for L B A Doing the multiplication: and make a Taylor Series of φ B. Then: [ φ A δa B + i ] δω µνs µν A B [φ B x µ φ A x ν δω µν ] Hence: φ A φ A µ φx ν δω µν + i δω µνs µν B A φ B δφ = [ ] i Sµν A B φ B µ φ A x ν δω µν Now for K µ. To determine this, we need to look at the change in the Lagrangian: Therefore: We can write this as: Lx LΛ 1 x Lx Lx µ δω µν x ν Lx Lx µ Lδω µν x ν δl = µ Lδω µν x ν δl = µ x ν Lδω µν Why? We can recover the original equation by doing the derivative with the product rule. One derivative will give a metric, which we use to change the differential to δω µ µ. This represents the trace of an antisymmetric matrix, which vanishes. The other term is the original equation. Next, we bring δω inside the derivative as well. We can treat this as a constant term because it is a differential: taking the derivative of a differential will effectively give a second-order differential, which we neglect. Then, Next we swap the indices: which gives, by the definition of K µ : δl = µ x ν Lδω µν δl = µ x ν Lδω µν K µ = δω µν x ν L Finally, we combine and into , the result is changing the indices as needed: j ρ = Lx [ ] i ρ φ A x Sµν A B φ B µ φ A x ν δω µν + Lδω ρν x ν 6
7 We distribute the first term: j ρ = Lx i ρ φ A x Sµν A B φ B µ φ A x ν Lx δω µν ρ φ A x + Lδωρν x ν This first term is B: j ρ = 1 Bρµν δω µν µ φ A x ν Lx δω µν ρ φ A x + Lδωρν x ν Using the result of part a, we have: j ρ = 1 Bρµν δω µν + T ρµ x ν δω µν g ρµ Lx ν δω µν + Lδω ρν x ν After manipulating the indices, these last two terms cancel: j ρ = 1 Bρµν δω µν + T ρµ x ν δω µν Rewriting this: j ρ = 1 [Bρµν δω µν T ρµ x ν δω µν T ρµ x ν δω µν ] In this last term, µ and ν are just dummy indices. We ll exchange them: j ρ = 1 [Bρµν δω µν T ρµ x ν δω µν T ρν x µ δω νµ ] δω is antisymmetric, so we can switch those indices: j ρ = 1 [Bρµν δω µν T ρµ x ν δω µν + T ρν x µ δω µν ] Now we factor out the differential: We recognize the term in the brackets as M: j ρ = 1 [Bρµν T ρµ x ν + T ρν x µ ] δω µν j ρ = 1 [Mρµν ] δω µν It is customary to drop the differential as well as the constant terms. Then, j ρµν = M ρµν as expected. c Use the conservation laws µ T µν = and µ M µνρ = to show that T νρ T ρν + µ B µνρ = 7
8 We have: This gives: µ M µνρ = µ x ν T µρ x ρ T µν + B µνρ = µ M µνρ = g ν µ T µρ + x ν µ T µ ρ g ρ µ T µν x ρ µ T µν + µ B µνρ = The derivative of T is zero, so: T νρ T ρν + µ B µνρ = d Define the improved energy-momentum tensor or Belinfante tensor i Show that Θ µν is symmetric. Θ µν = T µν + 1 ρb ρµν B µρν B νρµ We have: Θ µν = T µν + 1 ρ B ρµν B µρν B νρµ We can simply reorder these last two terms: Θ µν = T µν + 1 ρ B ρµν B νρµ B µρν From the definition of B, we see that the last two indices of B go onto S µν, the generators of the Lorentz Group for spinors. Since S is antisymmetric, it follows that B is antisymmetric in its last two indices. Therefore, we can write: We can even rewrite this as: Θ µν = T µν + 1 ρ B ρνµ B νρµ B µρν Θ µν = T µν ρ B ρνµ + 1 ρ B ρνµ B νρµ B µρν Again using the fact that B is antisymmetric in its last two indices, we write: Using the result from part c, we have: Θ µν = T µν + ρ B ρµν + 1 ρ B ρνµ B νρµ B µρν Θ µν = T νµ + 1 ρ B ρνµ B νρµ B µρν which gives: Θ µν = Θ νµ 8
9 ii Show that Θ µν is conserved, µ Θ µν = We take the derivative: µ Θ µν = µ T µν + 1 µ ρ B ρµν B µρν B νρµ This first term vanishes by Conservation of Energy. In the remaining terms, we will distribute: µ Θ µν = 1 µ ρ B ρµν 1 µ ρ B µρν 1 µ ρ B νρµ For the second term, we will use our usual trick of arbitrarily choosing to swap the dummy indices ρ and ν. Also, we ll divide the last term into two. These two changes give: µ Θ µν = 1 µ ρ B ρµν 1 ρ µ B ρµν 1 4 µ ρ B νρµ 1 4 µ ρ B νρµ Recall that partial derivatives commute; thus, the first and second terms cancel. fourth term, we ll again use our trick of swapping the dummy indices. Then: In the µ Θ µν = 1 4 µ ρ B νρµ 1 4 ρ µ B νµρ Now in the fourth term, we can again commute the partial derivatives. In addition, we have already discussed how B is antisymmetric in its last two indices. Thus, the remaining two terms cancel: µ Θ µν = iii Show that d 3 xθ ν = d 3 xt ν = P ν, where P ν is the energy-momentum four-vector. In general relativity, it is the Belinfante tensor that couples to gravity. We have: Θ ν d 3 x = T ν d 3 x + 1 ρ B ρν B ρν B νρ d 3 x We break this last term into temporal and spatial counterparts: Θ ν d 3 x = T ν d 3 x + 1 i B iν B iν B νi d 3 x + 1 B ν B ν B ν d 3 x The second integral on the right hand side vanishes, as it is an integral over a total divergence assuming reasonable boundary conditions at spatial infinity. In the last integral, the first two terms cancel, and the third term vanishes because B is antisymmetric in its last two indices, as discussed above. We re left with: Θ ν d 3 x = T ν d 3 x = P ν where the last equality follows by equation.35. e We define the improved tensor by: Ξ µνρ = x ν Θ µρ x ρ Θ µν 9
10 i Show that it obeys µ Ξ µνρ =. We evaluate the derivative: Using the product rule: µ Ξ µνρ = µ x ν Θ µρ x ρ Θ µν µ Ξ µνρ = µ x ν Θ µρ + x ν µ Θ µρ µ x ρ Θ µν x ρ µ Θ µν Since the Belinfante tensor is conserved our result from part d, the second and fourth terms vanish. In the remaining terms, we evaluate the derivative: Using the metric: µ Ξ µνρ = g ν µ Θ µρ g ρ µ Θ µν µ Ξ µνρ = Θ νρ Θ ρν Since the Belinfante Tensor is symmetric another result from part d, we have: µ Ξ µνρ = ii Show that d 3 xξ νρ = d 3 xm νρ = M νρ, where M νρ are the Lorentz generators. We have: [x Ξ νρ = ν Θ ρ x ρ Θ ν] Using the definition of Θ, we have: Ξ νρ d 3 x = [x ν T ρ + 1 [ µ B µρ B µρ B ρµ] x ρ T ν + 1 [ µ B µν B µν B νµ]] d 3 x Distributing: Ξ νρ d 3 x = x ν T ρ + 1 xν µ B µρ B µρ B ρµ x ρ T ν 1 xρ µ B µν B µν B νµ] d 3 x We break the sums over µ into temporal and spatial components: Ξ νρ d 3 x = x ν T ρ + 1 xν B ρ B ρ B ρ + 1 xν i B iρ B iρ B ρi x ρ T ν 1 xρ B ν B ν B ν 1 xρ i B iν B iν B νi] d 3 x The temporal terms vanish as before. Then: Ξ νρ d 3 x = x ν T ρ + 1 xν i B iρ B iρ B ρi x ρ T ν 1 xρ i B iν B iν B νi] d 3 x 1
11 Integrating by parts, we have: Ξ νρ d 3 x = x ν T ρ 1 ix ν B iρ B iρ B ρi x ρ T ν + 1 ix ρ B iν B iν B νi] d 3 x Doing the derivatives: Ξ νρ d 3 x = x ν T ρ 1 g ν i B iρ B iρ B ρi x ρ T ν + 1 g ρ i B iν B iν B νi] d 3 x Using the metric: Ξ νρ d 3 x = x ν T ρ 1 B νρ B νρ B ρν x ρ T ν + 1 B ρν B ρν B νρ] d 3 x The first and last terms cancel, as do the third and fourth. Then: Ξ νρ d 3 x = [x ν T ρ x ρ T ν + B νρ] d 3 x which is: Ξ νρ d 3 x = M νρ d 3 x = M νρ where the last equality follows by equation.4. f Compute Θ µν for a left-handed Weyl field with L given by equation 36., and for a Dirac field with L given by equation The Lagrangian given by equation 36. is: L = iψ ρ ρ ρ ψ 1 mψψ 1 mψ ψ where the m has been made real and positive as per the discussion in the text. We ve also changed the dummy index to ρ to avoid ambiguity later on. Then we can take the derivative: L µ ψ = iψ σ µ Equation gives, therefore: T µν = g µν [ iψ σ ρ ρ ψ 1 mψψ 1 mψ ψ ] iψ σ µ ν ψ Now we note that, since this is a left-handed Weyl Field, we take the generator of the Lorentz Group by equation 36.51: Equation 36.7 gives, therefore: S µν L B A = i 4 [σµ σ ν σ ν σ µ ] B A B µνρ = i 4 ψ σ µ [σ ν σ ρ σ ρ σ ν ] B A ψ B 11
12 Combining all these results in equation 36.7, we have: [ Θ µν = g µν iψ σ ρ ρ ψ 1 mψψ 1 ] mψ ψ iψ σ µ ν ψ + 1 [ i ρ 4 ψ A σ ρ [σ µ σ ν σ ρ σ ν ] B A ψ B i 4 ψ A σ µ [σ ρ σ ν σ ρ σ ν ] B A ψ B i 4 ψ A σ ν [σ ρ σ µ σ ρ σ ν ] B A ψ B There s not much we can do to simplify this. We could commute the derivative through the σ, but that would require us to use the product rule, making this more complicated rather than less so; further, nothing would cancel. All we can really do is to pull out some common factors: Θ µν = ig µν ψ σ ρ ρ ψ m gµν ψψ m gµν ψ ψ iψ σ µ ν ψ + i [ 8 ρ ψ A σ ρ σ µ σ ν σ ν σ µ B A ψ B ψ A σ µ σ ρ σ ν σ ν σ ρ B A ψ B ψ A σ ν σ ρ σ µ σ µ σ ρ B A ψ B ] ] As for the Dirac Field, we again have: The energy-momentum tensor is: Θ µν = T µν 1 ρ B ρµν B µρν B νρµ T µν = g µν L The Lagrangian is given by equation 36.8: and so we can compute L µ Ψ ν Ψ L = iψγ µ µ Ψ mψψ L µ Ψ = iψγµ Thus the energy-momentum tensor is given by: Finally, we need B µνρ, which is given by: T µν = ig µν Ψγ µ µ Ψ mg µν ΨΨ iψγ µ ν Ψ B µνρ = Ψ A γ µ S µν B A Ψ B where S µν is given by: S µν = +S µν L c a S µν R ȧċ 1
13 Combining our boxed results into equation gives us the explicit form for the Belinfante tensor. While it is normally worth writing these results explicitly, doing so in this case promises to yield a horrible equation which will yield very little insight. As such, it is perhaps better to leave our result in this form. Srednicki Symmetries of fermion fields. Consider a theory with N massless Weyl fields ψ j L = iψ j σµ µ ψ j where the repeated index j is summed. under the UN transformation, ψ j U jk ψ k This Lagrangian is clearly invariant where U is a unitary matrix. State the invariance group for the following cases: a N Weyl fields with a common mass M. Let s see if it s still true for UN: This becomes: L = iψ σ µ µ ψ m ψψ m ψ ψ L iu ij ψ j σ µ µ U ik ψ k m U ijψ j U ik ψ k m U ijψ j U ik ψ k L iψ U σ µ µ Uψ m ψ ju T jiu ik ψ k m ψ j U jiu ik ψ k Now we need to kill the Us. In the first term, as Srednicki says, the terms vanish if U U = 1. By the way, don t be concerned about commutation with the Pauli matrix: the Pauli matrix is multiplied by the derivative; the result is a ket of derivatives, which is an operator. This will commute with the constant unitary matrix. We ll soon develop a new notation to make this point cleaner. In the second and third terms, we need U T U = I in order to kill the Us; this implies that U T = U 1, which by our first condition implies that U T = U. This implies that U = U, which means that U must be real. A real unitary matrix is called an orthogonal matrix, and so the group is invariant under ON. b N massless Majorana fields L = i ΨT j Cγ µ µ Ψ j We can break the Majorana field into components of its Weyl fields. A Majorana field consists of only one Weyl field the left-handed one on top, and the conjugate of the right-handed 13
14 one on the bottom. Expanding the expression in the Lagrangian, we then get only N unique terms, the same as when we dealt directly with Weyl fields though there is now a factor of two, since the Weyl field appears twice per Majorana Field. The Lagrangian is then substantially unchanged from that of the first term of part a, and so is the symmetry group. UN. c N Majorana fields with a common mass m L = i ΨT j Cγ µ µ Ψ j 1 mψt j CΨ j Same as part b, except now the entire Lagrangian of part a is applicable, not merely the first term. The result is the same. ON. d N massless Dirac fields L = iψ j γ µ µ Ψ j Same as part b, except now there are two N mass terms in the Lagrangian rather than N, since each Dirac field consists of two Weyl spinors. All of these terms can mix together. Hence, the group is enlarged to UN. e N Dirac fields with a common mass m L = iψ j γ µ µ Ψ j mψ j Ψ j Same as part c, except now there are twice as many terms, since each Dirac field consists of two Weyl spinors. ON. 14
Srednicki Chapter 55
Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third
Διαβάστε περισσότερα6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Διαβάστε περισσότεραSpace-Time Symmetries
Chapter Space-Time Symmetries In classical fiel theory any continuous symmetry of the action generates a conserve current by Noether's proceure. If the Lagrangian is not invariant but only shifts by a
Διαβάστε περισσότεραderivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
Διαβάστε περισσότερα= {{D α, D α }, D α }. = [D α, 4iσ µ α α D α µ ] = 4iσ µ α α [Dα, D α ] µ.
PHY 396 T: SUSY Solutions for problem set #1. Problem 2(a): First of all, [D α, D 2 D α D α ] = {D α, D α }D α D α {D α, D α } = {D α, D α }D α + D α {D α, D α } (S.1) = {{D α, D α }, D α }. Second, {D
Διαβάστε περισσότεραPhys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Διαβάστε περισσότεραHOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:
HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying
Διαβάστε περισσότεραSection 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Διαβάστε περισσότεραCHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
Διαβάστε περισσότεραLecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all
Διαβάστε περισσότεραMath221: HW# 1 solutions
Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin
Διαβάστε περισσότερα3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β
3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle
Διαβάστε περισσότεραC.S. 430 Assignment 6, Sample Solutions
C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order
Διαβάστε περισσότεραSymmetric Stress-Energy Tensor
Chapter 3 Symmetric Stress-Energy ensor We noticed that Noether s conserved currents are arbitrary up to the addition of a divergence-less field. Exploiting this freedom the canonical stress-energy tensor
Διαβάστε περισσότερα2 Composition. Invertible Mappings
Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,
Διαβάστε περισσότεραMATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)
1. MATH43 String Theory Solutions 4 x = 0 τ = fs). 1) = = f s) ) x = x [f s)] + f s) 3) equation of motion is x = 0 if an only if f s) = 0 i.e. fs) = As + B with A, B constants. i.e. allowe reparametrisations
Διαβάστε περισσότεραProblem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.
Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +
Διαβάστε περισσότεραSection 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
Διαβάστε περισσότεραExample Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Διαβάστε περισσότεραTutorial problem set 6,
GENERAL RELATIVITY Tutorial problem set 6, 01.11.2013. SOLUTIONS PROBLEM 1 Killing vectors. a Show that the commutator of two Killing vectors is a Killing vector. Show that a linear combination with constant
Διαβάστε περισσότεραHomework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
Διαβάστε περισσότεραSolutions to Exercise Sheet 5
Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X
Διαβάστε περισσότεραPartial Differential Equations in Biology The boundary element method. March 26, 2013
The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet
Διαβάστε περισσότεραHomework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Διαβάστε περισσότεραMatrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Διαβάστε περισσότεραJesse Maassen and Mark Lundstrom Purdue University November 25, 2013
Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering
Διαβάστε περισσότεραHomework 4 Solutions Weyl or Chiral representation for γ-matrices. Phys624 Dirac Equation Homework 4
Homework 4 Solutions 4.1 - Weyl or Chiral representation for γ-matrices 4.1.1: Anti-commutation relations We can write out the γ µ matrices as where ( ) 0 σ γ µ µ = σ µ 0 σ µ = (1, σ), σ µ = (1 2, σ) The
Διαβάστε περισσότεραΑπόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Διαβάστε περισσότεραProblem Set 3: Solutions
CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C
Διαβάστε περισσότεραforms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with
Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We
Διαβάστε περισσότεραEE512: Error Control Coding
EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3
Διαβάστε περισσότεραSecond Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
Διαβάστε περισσότεραHigher Derivative Gravity Theories
Higher Derivative Gravity Theories Black Holes in AdS space-times James Mashiyane Supervisor: Prof Kevin Goldstein University of the Witwatersrand Second Mandelstam, 20 January 2018 James Mashiyane WITS)
Διαβάστε περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραFinite Field Problems: Solutions
Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The
Διαβάστε περισσότεραExercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.
Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given
Διαβάστε περισσότεραPhys624 Quantization of Scalar Fields II Homework 3. Homework 3 Solutions. 3.1: U(1) symmetry for complex scalar
Homework 3 Solutions 3.1: U(1) symmetry for complex scalar 1 3.: Two complex scalars The Lagrangian for two complex scalar fields is given by, L µ φ 1 µ φ 1 m φ 1φ 1 + µ φ µ φ m φ φ (1) This can be written
Διαβάστε περισσότεραSCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
Διαβάστε περισσότερα9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr
9.9 #. Area inside the oval limaçon r = + cos. To graph, start with = so r =. Compute d = sin. Interesting points are where d vanishes, or at =,,, etc. For these values of we compute r:,,, and the values
Διαβάστε περισσότεραΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο
Διαβάστε περισσότεραb. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!
MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.
Διαβάστε περισσότεραConcrete Mathematics Exercises from 30 September 2016
Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)
Διαβάστε περισσότερα( y) Partial Differential Equations
Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate
Διαβάστε περισσότεραPractice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1
Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the
Διαβάστε περισσότεραOrbital angular momentum and the spherical harmonics
Orbital angular momentum and the spherical harmonics March 8, 03 Orbital angular momentum We compare our result on representations of rotations with our previous experience of angular momentum, defined
Διαβάστε περισσότεραOrdinal Arithmetic: Addition, Multiplication, Exponentiation and Limit
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal
Διαβάστε περισσότεραDirac Matrices and Lorentz Spinors
Dirac Matrices and Lorentz Spinors Background: In 3D, the spinor j = 1 representation of the Spin3) rotation group is constructed from the Pauli matrices σ x, σ y, and σ k, which obey both commutation
Διαβάστε περισσότερα1 String with massive end-points
1 String with massive end-points Πρόβλημα 5.11:Θεωρείστε μια χορδή μήκους, τάσης T, με δύο σημειακά σωματίδια στα άκρα της, το ένα μάζας m, και το άλλο μάζας m. α) Μελετώντας την κίνηση των άκρων βρείτε
Διαβάστε περισσότεραFourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics
Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)
Διαβάστε περισσότερα4.6 Autoregressive Moving Average Model ARMA(1,1)
84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this
Διαβάστε περισσότεραST5224: Advanced Statistical Theory II
ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known
Διαβάστε περισσότεραCRASH COURSE IN PRECALCULUS
CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter
Διαβάστε περισσότεραChapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Διαβάστε περισσότερα( ) 2 and compare to M.
Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8
Διαβάστε περισσότεραPARTIAL NOTES for 6.1 Trigonometric Identities
PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot
Διαβάστε περισσότεραPartial Trace and Partial Transpose
Partial Trace and Partial Transpose by José Luis Gómez-Muñoz http://homepage.cem.itesm.mx/lgomez/quantum/ jose.luis.gomez@itesm.mx This document is based on suggestions by Anirban Das Introduction This
Διαβάστε περισσότεραFinite difference method for 2-D heat equation
Finite difference method for 2-D heat equation Praveen. C praveen@math.tifrbng.res.in Tata Institute of Fundamental Research Center for Applicable Mathematics Bangalore 560065 http://math.tifrbng.res.in/~praveen
Διαβάστε περισσότεραk A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +
Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b
Διαβάστε περισσότεραOther Test Constructions: Likelihood Ratio & Bayes Tests
Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :
Διαβάστε περισσότεραANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?
Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least
Διαβάστε περισσότεραEvery set of first-order formulas is equivalent to an independent set
Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent
Διαβάστε περισσότεραD Alembert s Solution to the Wave Equation
D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique
Διαβάστε περισσότεραMA 342N Assignment 1 Due 24 February 2016
M 342N ssignment Due 24 February 206 Id: 342N-s206-.m4,v. 206/02/5 2:25:36 john Exp john. Suppose that q, in addition to satisfying the assumptions from lecture, is an even function. Prove that η(λ = 0,
Διαβάστε περισσότεραThe Simply Typed Lambda Calculus
Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and
Διαβάστε περισσότεραDESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.
DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec
Διαβάστε περισσότεραSymmetry. March 31, 2013
Symmetry March 3, 203 The Lie Derivative With or without the covariant derivative, which requires a connection on all of spacetime, there is another sort of derivation called the Lie derivative, which
Διαβάστε περισσότεραHomework 3 Solutions
Homework 3 s Free graviton Hamiltonian Show that the free graviton action we discussed in class (before making it gauge- and Lorentzinvariant), S 0 = α d 4 x µ h ij µ h ij, () yields the correct free Hamiltonian
Διαβάστε περισσότεραRight Rear Door. Let's now finish the door hinge saga with the right rear door
Right Rear Door Let's now finish the door hinge saga with the right rear door You may have been already guessed my steps, so there is not much to describe in detail. Old upper one file:///c /Documents
Διαβάστε περισσότεραVariational Wavefunction for the Helium Atom
Technische Universität Graz Institut für Festkörperphysik Student project Variational Wavefunction for the Helium Atom Molecular and Solid State Physics 53. submitted on: 3. November 9 by: Markus Krammer
Διαβάστε περισσότεραDERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C
DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C By Tom Irvine Email: tomirvine@aol.com August 6, 8 Introduction The obective is to derive a Miles equation which gives the overall response
Διαβάστε περισσότεραNon-Abelian Gauge Fields
Chapter 5 Non-Abelian Gauge Fields The simplest example starts with two Fermions Dirac particles) ψ 1, ψ 2, degenerate in mass, and hence satisfying in the absence of interactions γ 1 i + m)ψ 1 = 0, γ
Διαβάστε περισσότεραSection 9.2 Polar Equations and Graphs
180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify
Διαβάστε περισσότεραECE Spring Prof. David R. Jackson ECE Dept. Notes 2
ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =
Διαβάστε περισσότερα= λ 1 1 e. = λ 1 =12. has the properties e 1. e 3,V(Y
Stat 50 Homework Solutions Spring 005. (a λ λ λ 44 (b trace( λ + λ + λ 0 (c V (e x e e λ e e λ e (λ e by definition, the eigenvector e has the properties e λ e and e e. (d λ e e + λ e e + λ e e 8 6 4 4
Διαβάστε περισσότεραTridiagonal matrices. Gérard MEURANT. October, 2008
Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,
Διαβάστε περισσότεραTMA4115 Matematikk 3
TMA4115 Matematikk 3 Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet Trondheim Spring 2010 Lecture 12: Mathematics Marvellous Matrices Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet
Διαβάστε περισσότεραNotes on the Open Economy
Notes on the Open Econom Ben J. Heijdra Universit of Groningen April 24 Introduction In this note we stud the two-countr model of Table.4 in more detail. restated here for convenience. The model is Table.4.
Διαβάστε περισσότεραF-TF Sum and Difference angle
F-TF Sum and Difference angle formulas Alignments to Content Standards: F-TF.C.9 Task In this task, you will show how all of the sum and difference angle formulas can be derived from a single formula when
Διαβάστε περισσότεραTrigonometry 1.TRIGONOMETRIC RATIOS
Trigonometry.TRIGONOMETRIC RATIOS. If a ray OP makes an angle with the positive direction of X-axis then y x i) Sin ii) cos r r iii) tan x y (x 0) iv) cot y x (y 0) y P v) sec x r (x 0) vi) cosec y r (y
Διαβάστε περισσότεραReminders: linear functions
Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U
Διαβάστε περισσότεραNumerical Analysis FMN011
Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =
Διαβάστε περισσότεραMath 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.
Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequalit for metrics: Let (X, d) be a metric space and let x,, z X. Prove that d(x, z) d(, z) d(x, ). (ii): Reverse triangle inequalit for norms:
Διαβάστε περισσότεραApproximation of distance between locations on earth given by latitude and longitude
Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth
Διαβάστε περισσότεραPHYS606: Electrodynamics Feb. 01, Homework 1. A νµ = L ν α L µ β A αβ = L ν α L µ β A βα. = L µ β L ν α A βα = A µν (3)
PHYS606: Electrodynamics Feb. 01, 2011 Instructor: Dr. Paulo Bedaque Homework 1 Submitted by: Vivek Saxena Problem 1 Under a Lorentz transformation L µ ν, a rank-2 covariant tensor transforms as A µν A
Διαβάστε περισσότεραThe kinetic and potential energies as T = 1 2. (m i η2 i k(η i+1 η i ) 2 ). (3) The Hooke s law F = Y ξ, (6) with a discrete analog
Lecture 12: Introduction to Analytical Mechanics of Continuous Systems Lagrangian Density for Continuous Systems The kinetic and potential energies as T = 1 2 i η2 i (1 and V = 1 2 i+1 η i 2, i (2 where
Διαβάστε περισσότεραExercises to Statistics of Material Fatigue No. 5
Prof. Dr. Christine Müller Dipl.-Math. Christoph Kustosz Eercises to Statistics of Material Fatigue No. 5 E. 9 (5 a Show, that a Fisher information matri for a two dimensional parameter θ (θ,θ 2 R 2, can
Διαβάστε περισσότερα6.3 Forecasting ARMA processes
122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear
Διαβάστε περισσότεραw o = R 1 p. (1) R = p =. = 1
Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:
Διαβάστε περισσότεραRiemannian Curvature
Riemannian Curvature February 6, 013 We now generalize our computation of curvature to arbitrary spaces. 1 Parallel transport around a small closed loop We compute the change in a vector, w, which we parallel
Διαβάστε περισσότεραCHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3
Διαβάστε περισσότεραDifferential equations
Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential
Διαβάστε περισσότεραLecture 2. Soundness and completeness of propositional logic
Lecture 2 Soundness and completeness of propositional logic February 9, 2004 1 Overview Review of natural deduction. Soundness and completeness. Semantics of propositional formulas. Soundness proof. Completeness
Διαβάστε περισσότεραUniform Convergence of Fourier Series Michael Taylor
Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula
Διαβάστε περισσότεραLecture 34 Bootstrap confidence intervals
Lecture 34 Bootstrap confidence intervals Confidence Intervals θ: an unknown parameter of interest We want to find limits θ and θ such that Gt = P nˆθ θ t If G 1 1 α is known, then P θ θ = P θ θ = 1 α
Διαβάστε περισσότεραORDINAL ARITHMETIC JULIAN J. SCHLÖDER
ORDINAL ARITHMETIC JULIAN J. SCHLÖDER Abstract. We define ordinal arithmetic and show laws of Left- Monotonicity, Associativity, Distributivity, some minor related properties and the Cantor Normal Form.
Διαβάστε περισσότεραEcon 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1
Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test
Διαβάστε περισσότερα4 Dirac Equation. and α k, β are N N matrices. Using the matrix notation, we can write the equations as imc
4 Dirac Equation To solve the negative probability density problem of the Klein-Gordon equation, people were looking for an equation which is first order in / t. Such an equation is found by Dirac. It
Διαβάστε περισσότεραStatistical Inference I Locally most powerful tests
Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided
Διαβάστε περισσότεραInverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
Διαβάστε περισσότερα