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Solution Manual for An Introduction to Groups and their Matrices for Science Students 1st Edition By

Page 1

1.1 Apply Tx = −x. Tx = −x Te x = e(−x) = e−x Here is another approach. Apply the operator to e x expressed in series form. ! x2 x3 x + + ... Te = T 1 + x + 2! 3! ! (−x)2 (−x)3 + + ... = 1−x+ 2! 3! ! x2 x3 = 1−x+ − + ... 2! 3! = e−x The operator has changed the sign of the odd terms.


2

FUNDAMENTAL CONCEPTS

1.2 Apply Tx = −x. T cos (x) = cos (−x) = cos (x) This result can also be understood by considering the series expansion of cos (x). x2 x4 x6 + − + ... 2! 4! 6! T cos (x) = cos (−x) cos (x) = 1 −

(−x)2 (−x)4 (−x)6 + − + ... 2! 4! 6! x2 x4 x6 =1− + − + ... 2! 4! 6! = cos (x) =1−

The series expansion of cos (x) contains only even terms, so Tx = −x changes nothing.

1.3 According to the group axioms (AB)(AB)−1 = E Multiply by A−1 from the left.

A−1 AB(AB)−1 = A−1 E B(AB)−1 = A−1 Multiply by B−1 from the left.

B−1 B(AB)−1 = B−1 A−1 (AB)−1 = B−1 A−1


FUNDAMENTAL CONCEPTS

3

1.4 Check whether the axioms that define a group (Sec. (1.3) of the text) are satisfied for positive and negative real integers under addition. The sum of two integers is also an integer, a member of the set, satisfying axiom (ii) that the group operation does not result in an element outside the set. The sum of an integer N and 0 is equal to N, so 0 acts as the identity element under addition, satisfying axiom (iii) that the group must have an identity element. The sum of an integer N and its negative −N is N − N, equal to the identity element 0. Every integer N has an inverse element −N under addition, so axiom (iv) is satisfied that the group must contain an inverse under the group operation for every element. Trivially, the addition of integers is associative: N1 + (N2 + N3 ) = (N1 + N2 ) + N3 , satisfying axiom(v).

1.5 Check whether the axioms that define a group (Sec. (1.3) of the text) are satisfied by the set of real integers under multiplication. The product of two integers is also an integer, a member of the set, satisfying axiom (ii) that the group operation does not result in an element outside the set. The product of an integer N and 1 is equal to N, so 1 acts as the identity element under multiplication, satisfying axiom (iii) that the group must have an identity element. Axiom (iv) requires that N × N −1 = 1. It follows that N −1 = N1 . The inverse of a real integer under multiplication is not an integer except for 1, so the real integers are not a group because the set of real integers does not include the inverses under multiplication.


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FUNDAMENTAL CONCEPTS

1.6 The product table for the group {E, A, B} is E E A B

E A B

A A B E

B B E A

The product table shows that B2 = BB = A. Hence the cyclic set {E, B, B2 } has the same elements as the set {E, B, A}.

1.7 The group must have an identity element E. Let the group’s two elements be E and A, where A is distinct from E. A2 can only be A or E. If A2 = A, then A2 = A AA = A Multiplying by A−1 from the left gives

A=E so for this case A = E and A is not distinct. Hence the only possibility is AA = E so the product table must be E A

E E A

A A E


FUNDAMENTAL CONCEPTS

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1.8 Products of the operations can be found by adding their rotations. For example, CC = 270◦ + 270◦ = 540◦ = 180◦ + 360◦ = BE = B. EE = 0◦ + 0◦ = E

EA = 0◦ + 90◦ = A

EB = 0◦ + 180◦ = B

EC = 0◦ + 270◦ = C

AE = 90◦ + 0◦ = A

AA = 90◦ + 90◦ = B

AB = 90◦ + 180◦ = C

AC = 90◦ + 270◦ = E

BE = 180◦ + 0◦ = B

BA = 180◦ + 90◦ = C BB = 180◦ + 180◦ = E

BC = 180◦ + 270◦ = A

CE = 270◦ + 0◦ = C CA = 270◦ + 90◦ = E CB = 270◦ + 180◦ = A CC = 270◦ + 270◦ = B

The product table is therefore E E A B C

E A B C

A A B C E

B B C E A

C C E A B

The group is cyclic – for example AE = A AA = B AB = AAA = C AC = AAAA = E and similarly for the other group elements.

1.9 Consider the hypothetical product table for the group of distinct operations {E, P, Q, R} where the Q column contains the operation P twice. E P Q R

E E P Q R

P P Q R E

Q Q R P P

R R E P Q

According to the product table QQ = P RQ = P QQ = RQ Multiplying by Q−1 from the right gives Q = R. This is a contradiction because the operations are assumed to be distinct.


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FUNDAMENTAL CONCEPTS

1.10 The product table for S3 is E P2 P3 P4 P5 P6

E E P2 P3 P4 P5 P6

P2 P2 E P5 P6 P3 P4

P3 P3 P6 E P5 P4 P2

P4 P4 P5 P6 E P2 P3

P5 P5 P4 P2 P3 P6 E

P6 P6 P3 P4 P3 E P5

According to the product table for S3 the set {E, P5 , P6 } has the product table E E P5 P6

E P5 P6

P5 P5 P6 E

P6 P6 E P5

The set {E, P5 , P6 } satisfies the group axioms. Cayley’s theorem says that S 3 has every subgroup of order 3. {E, P5 , P6 } is the only subgroup of order 3 found in S3 and there are no others.

1.11

E K L M

E E K L M

K K E M L

L L M E K

M M L K E

Check that the group axioms are satisfied: (ii) The product of any two operations is a member of the set. (iii) There is an identity element E such that KE = K, etc. (iv) Every element of the set has an inverse. KK = E so that K−1 = K etc. The group is Abelian; all the elements commute. KL = LK = M etc. The group is not cyclic. K2 = E etc. The group elements cannot be obtained by taking powers of one element.


FUNDAMENTAL CONCEPTS

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1.12 The product table for a group {E, A} of order 2 is E A

E E A

A A E

For distinct elements it follows that AA = E. Inspection of the product table for S3 (see Problem 1.10) shows that Pn Pn = E for n = 2, 3, 4. The three subgroups of order 2 are therefore {E, P2 }, {E, P3 } and {E, P4 }.

1.13 (a)   1 2 3   2 3 1 For the interchange 3 ↔ 1 the bottom row becomes (213). A second interchange 2 ↔ 1 converts the bottom row to standard form (123). Because two interchanges are required, this permutation is even. (b)   1 2 3 4   2 3 1 4 For the interchange 3 ↔ 1 the bottom row becomes (2134). A second interchange 2 ↔ 1 converts the bottom row to standard form (1234). Because two interchanges are required, this permutation is even. (c)   1 2 3 4   4 3 2 1 Converting to standard form requires 2 interchanges: 4 ↔ 1. The bottom row becomes (1324). 3 ↔ 2. The bottom row becomes (1234). This permutation is even.


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FUNDAMENTAL CONCEPTS

1.14 In cycle notation for permutations an entry maps the entry on its right. Hence for the cycle (536142), 6 7→ 1.

1.15 In cycle notation the entry at the end of the cycle maps around to the entry at the beginning. Hence for the cycle (326415), 5 7→ 3.

1.16

Let c be the length of the side of the equilateral triangle. The “flip” in this problem is a rotation about aa by π. Before the flip the coordinates are √ 3 xt = 0, yt = 2 c (top apex) xr = 2c , yr = 0 (bottom right apex) x` = − 2c , y` = 0 (bottom left apex) After the flip√the coordinates are xt0 = 0, y0t = 23 c xr0 = − 2c , y0r = 0 x`0 = + 2c , y0` = 0 continued next page =⇒


FUNDAMENTAL CONCEPTS

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The representation matrix has the general form ! ! ! A11 A12 xi xi0 = A21 A22 yi y0i

Written out, the matrix form is xi0 = A11 xi + A12 yi y0i = A21 xi + A22 yi To start evaluating the terms Ai j , note that y0i is independent of xi . Therefore A21 = 0. Because y0i = yi , A22 = 1. Similarly A12 = 0 because xi0 is independent of yi . A11 = −1 because xr and x` change sign from the flip. The result for the representation matrix is   −1 0   0 1

1.17 The product table for the group Γ = {E, A, B} is

E A B

E E A B

A A B E

B B E A

A correct homomorphism must give product results that agree with the product table. For example, according to the product table AB = E. The corresponding homomorphism product (-1) (-1) = (1) agrees. However, AA = B. The homomorphism (-1) (-1) = (1) does not agree. The given matrices are not a homomorphism for Γ.


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FUNDAMENTAL CONCEPTS

1.18 Consider C = AB where A and B are n × n diagonal matrices. The elements of A and B satisfy Ai j = 0

i, j

Bk` = 0

k,`

The elements of C are Ci` =

n X

Ai j B j`

j

Ai j = 0 if i , j.

Ci` = Aii Bi` Bi` = 0 if i , ` so C has only diagonal elements Cii = Aii Bii .

1.19 The group operations are E: rotate by 0◦ A: rotate by 90◦ B: rotate by 180◦ C: rotate by 270◦ The required matrix was derived in Sec. (1.5.3).    cos θ sin θ    − sin θ cos θ   1 0   0 1

   0 1   −1 0

  −1 0    0 −1

  0 −1   1 0

D(E)

D(A)

D(B)

D(C)


FUNDAMENTAL CONCEPTS

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1.20 A matrix has an inverse only if its determinant is not 0. Otherwise, it would be possible to use Cramer’s rule to calculate an inverse. (a) det

1 0 = (1)(−1) = −1 0 −1

This matrix has an inverse. (b) det

1 −1 = (1)(−1) − (1)(−1) = 0 1 −1

This matrix does not have an inverse. (c) 1 3 2 det 3 0 −1 = (1)(−2) − (3)(3 + 2) + (2)(−6) = −29 2 −2 1 This matrix has an inverse.


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FUNDAMENTAL CONCEPTS

1.21 Let C be the resultant matrix in each case. C = A+B Ci j = Ai j + Bi j      3 2 −3  5 2 −3     C = −2 3 2  +  1 3 1      1 0 4 −2 0 5    8 4 −6   = −1 6 3    −1 0 9 C = A−B Ci j = Ai j − Bi j   −2 0 0    C = −3 0 1    3 0 −1 C = AB X Ci j = Aik Bk j k

  (3)(5) + (2)(1) + (−3)(−2) (3)(2) + (2)(3) + 0 (3)(−3) + (2)(1) + (−3)(5)   C = (−2)(5) + (3)(1) + (2)(−2) (−2)(2) + (3)(3) + 0 (−2)(−3) + (3)(1) + (2)(5)   (1)(5) + 0 + (4)(−2) (1)(2) + 0 + 0 (1)(−3) + 0 + (4)(5)    23 12 −22   = −11 5 19    −3 2 17 C = BA X Ci j = Bik Ak j k

  (5)(3) + (2)(−2) + (−3)(1) (5)(2) + (2)(3) + 0 (5)(−3) + (2)(2) + (−3)(4)   C =  (1)(3) + (3)(−2) + (1)(1) (1)(2) + (3)(3) + 0 (1)(−3) + (3)(2) + (1)(4)    (−2)(3) + 0 + (5)(1) (−2)(2) + 0 + 0 (−2)(−3) + 0 + (5)(4)    8 16 −23   = −2 11 7    −1 −4 26


FUNDAMENTAL CONCEPTS

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1.22

Let C be the resultant matrix in each case.

C = A+B Ci j = Ai j + Bi j     −1 5 4   2 −2 −1     C = −3 3 4  +  5 1 4      2 0 −3 −3 0 2    1 3 3    =  2 4 8    −1 0 −1 C = A−B Ci j = Ai j − Bi j   −3 7 5    C = −8 2 0    5 0 −5 C = AB X Ci j = Aik Bk j k

  (−1)(2) + (5)(5) + (4)(−3) (−1)(−2) + (5)(1) + 0 (−1)(−1) + (5)(4) + (4)(2)   C = (−3)(2) + (3)(5) + (4)(−3) (−3)(−2) + (3)(1) + 0 (−3)(−1) + (3)(4) + (4)(2)   (2)(2) + 0 + (−3)(−3) (2)(−2) + 0 + 0 (2)(−1) + 0 + (−3)(2)    11 7 29    = −3 9 23    13 −4 −8 C = BA X Ci j = Bik Ak j k

  (2)(−1) + (−2)(−3) + (−1)(2) (2)(5) + (−2)(3) + 0 (2)(4) + (−2)(4) + (−1)(−3)   C =  (5)(−1) + (1)(−3) + (4)(2) (5)(5) + (1)(3) + 0 (5)(4) + (1)(4) + (4)(−3)    (−3)(−1) + 0 + (2)(2) (−3)(5) + 0 + 0 (−3)(4) + 0 + (2)(−3)   2 4 3    = 0 28 12    7 −15 −18


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FUNDAMENTAL CONCEPTS

1.23

 2  A = 2  3  1  B = 0  2  6  AB = 8  1

 −1 2   0 3   −1 −1  2 −2  3 −1  1 −2  3 −7   7 −10  2 −3

det(A) = (2)(3) − (−1)(−11) + (2)(−2) = −9 det(B) = (1)(−5) − (2)(2) + (−2)(−6) =3 det(A) det(B) = (−9)(3) = −27 det(AB) = (6)(−1) − (3)(−14) + (−7)(9) = −27

1.24 Ã is the transpose of matrix A so its elements are (Ã)i j = A ji . f i j = (AB) ji (AB) X = A jk Bki =

k X

Ãk j B̃ik

k

=

X k

= B̃Ã

B̃ik Ãk j


FUNDAMENTAL CONCEPTS

1.25

  1 5 2    A = 3 0 −1   4 −2 1 (A∗ )i j = A∗i j   1 5 2    = 3 0 −1   4 −2 1 (Ã)i j = A ji   1 3 4    = 5 0 −2   2 −1 1 (A† )i j = (A∗ ) ji   1 3 4    = 5 0 −2   2 −1 1

15


16

FUNDAMENTAL CONCEPTS

1.26

   1 3+i 2i    A =  3 0 −1 + 2i   4 − 3i −2 1−i (A∗ )i j = A∗i j    1 3−i −2i    =  3 0 −1 − 2i   4 + 3i −2 1+i (Ã)i j = A ji    1 3 4 − 3i   = 3 + i 0 −2    2i −1 + 2i 1 − i (A† )i j = (A∗ ) ji    1 3 4 + 3i   = 3 − i 0 −2    −2i −1 − 2i 1 + i


2.1 In the problem the reference to Sec. (1.4) should instead be to Sec. (1.5.3). Let T be rotation by θ and let φ1 = x, φ2 = y.If x and y are truly basis functions for this operation they must satisfy Tφ j = Tx = D11 x + D12 y Tφ2 = Ty = D21 x + D22 y In Sec.(1.5.3) Eqs. (1.1) and (1.2), the expression for rotation of the x − y axes is Tx = x cos θ + y sin θ Ty = −x sin θ + y cos θ The operation of T on x and y give terms involving only x and y. Hence x and y qualify as basis functions. continued next page =⇒


18

MATRIX REPRESENTATIONS OF DISCRETE GROUPS

D11 = cos θ D12 = sin θ D21 = − sin θ D22 = cos θ    cos θ sin θ   D(T) =  − sin θ cos θ This is the same as the matrix in Sec. (1.5.3) for rotated axes. The matrix D(T) for θ = 120◦ is therefore √   3  − 1  2 2   √ D(T) =  3 1 − 2 −2

2.2 In the problem the reference to Sec. (1.4) should instead be to Sec. (1.5.3). In Sec.(1.5.3) Eqs. (1.1) and (1.2), the expression for rotation of the x − y axes is Tx = x cos θ + y sin θ Ty = −x sin θ + y cos θ Tx2 = (x cos θ + y sin θ)2 = x2 cos2 θ + y2 sin2 θ + 2xy cos θ sin θ Ty2 = (−x sin θ + y cos θ)2 = x2 sin2 θ + y2 cos2 θ − 2xy cos θ sin θ T(x2 − y2 ) = (x2 − y2 )(cos2 θ − sin2 θ) + 4xy cos θ sin θ T(xy) = (x cos θ + y sin θ)(−x sin θ + y cos θ) = −(x2 − y2 ) cos θ sin θ + xy(cos2 θ − sin2 θ) T(x2 −y2 ) and T(xy) contain only the functions (x2 −y2 ) and (xy) so these are indeed basis functions referring to the same subspace. continued next page =⇒


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