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Exercise: does the representation descend?

A representation ρ\rho of a group G~\widetilde G defines a representation of G~/Γ\widetilde G/\Gamma precisely when every element of Γ\Gamma acts as the identity. The exercises below turn this condition into parity, congruence, and topology checks. Work analytically before using the linked tools.

All representations here are finite-dimensional ordinary complex representations of compact connected groups. The Lie-algebra modules integrate uniquely to the stated simply connected compact groups. Descent to a further quotient is an additional requirement; it is not a change in the Lie-algebra action.

For SU(N)SU(N), N≥2N\geq2, use the AN−1A_{N-1} Dynkin order in which node rr labels ΛrCN\Lambda^r\mathbb C^N. For labels (a1,…,aN−1)(a_1,\ldots,a_{N-1}), put

b=∑r=1N−1rar,z=e2πi/NIN.b=\sum_{r=1}^{N-1}r a_r, \qquad z=e^{2\pi i/N}I_N.

Then zz acts by e2πib/Ne^{2\pi i b/N}. The order-kk subgroup Γk=⟨zN/k⟩\Gamma_k=\langle z^{N/k}\rangle, for k∣Nk\mid N, acts trivially exactly when b≡0(modk)b\equiv0\pmod k. This follows by testing its generator. The underlying highest-weight and central-quotient results are Etingof, §43.1, Theorem 43.4 and Corollary 43.5, pp. 231–232; the covers and global forms lesson develops the argument.

Let Vn=Sym⁡nC2V_n=\operatorname{Sym}^n\mathbb C^2 be the SU(2)SU(2) irrep with highest weight nn and spin j=n/2j=n/2.

  1. Determine the action of −I-I on VnV_n directly from its tensor construction.
  2. For n=1,2,3,4n=1,2,3,4, give the dimension and decide whether it descends through SU(2)→SO(3)SU(2)\to SO(3).
  3. Does a failed descent mean that the corresponding su(2)\mathfrak{su}(2) representation fails to exist?

The central element contributes one factor of −1-1 on each fundamental tensor factor, so it acts on VnV_n by (−1)n(-1)^n. The symmetric tensors have basis xn−ryrx^{n-r}y^r, r=0,…,nr=0,\ldots,n, giving dimension n+1n+1.

nn jj Dimension Central sign Descends to SO(3)SO(3)?
11 1/21/2 22 −1-1 No
22 11 33 +1+1 Yes
33 3/23/2 44 −1-1 No
44 22 55 +1+1 Yes

All four are valid Lie-algebra modules and SU(2)SU(2) group representations. Only the even-nn modules factor through the specified quotient as ordinary linear SO(3)SO(3) representations. This does not deny the separate projective interpretation of half-integer spin.

Check the doublet and triplet, and inspect the covering map.

2. Triality and reality are different tests

Section titled “2. Triality and reality are different tests”

For SU(3)SU(3), consider labels (p,q)=(1,0),(1,1),(3,0)(p,q)=(1,0),(1,1),(3,0).

  1. Compute p+2qp+2q modulo 33 and decide which representations descend to PSU(3)=SU(3)/Z3PSU(3)=SU(3)/\mathbb Z_3.
  2. Compute their dimensions using dim⁡(p,q)=(p+1)(q+1)(p+q+2)/2\dim(p,q)=(p+1)(q+1)(p+q+2)/2.
  3. Is every representation that descends necessarily self-conjugate?
Labels Triality Dimension Descends to PSU(3)PSU(3)?
(1,0)(1,0) 11 33 No
(1,1)(1,1) 00 88 Yes
(3,0)(3,0) 00 1010 Yes

Conjugation exchanges (p,q)(p,q) with (q,p)(q,p). Thus the 1010 with labels (3,0)(3,0) descends, although its conjugate (0,3)(0,3) is inequivalent. Descent tests a central kernel; self-conjugacy tests equivalence to the conjugate representation. They answer different questions.

The dimension formula and label convention are derived in roots and weights. Check the 10 of PSU(3) and the SU(3) quotient map.

Consider matter in the 6=Λ2C46=\Lambda^2\mathbb C^4 with labels (0,1,0)(0,1,0) and the adjoint 1515 with labels (1,0,1)(1,0,1). The center is generated by z=iI4z=iI_4.

  1. Find the subgroup of Z(SU(4))Z(SU(4)) acting trivially on both representations.
  2. Which quotients SU(4)/ΓkSU(4)/\Gamma_k, k∣4k\mid4, admit this matter content?
  3. What are the fundamental group and center of the largest such quotient?
  4. What changes if one fundamental 44 is added?

The 66 has b=2b=2, so zz acts as −1-1 and z2=−I4z^2=-I_4 acts as +1+1. This can also be seen without the label formula: a scalar ii on each of two exterior factors gives i2=−1i^2=-1. The adjoint has b=1+3=4b=1+3=4 and trivial center action; directly, scalar conjugation acts trivially on traceless matrices. Their common central kernel is therefore

K={I4,−I4}=⟨z2⟩≅Z2.K=\{I_4,-I_4\}=\langle z^2\rangle\cong\mathbb Z_2.

The admissible choices are k=1k=1 and k=2k=2. The 66 obstructs the full adjoint quotient PSU(4)PSU(4), whose kernel also contains iI4iI_4. Matter compatibility permits a choice among these groups; it does not require taking the largest kernel.

Because SU(4)SU(4) is simply connected,

π1(SU(4)/K)≅K≅Z2,Z(SU(4)/K)≅Z4/K≅Z2.\pi_1(SU(4)/K)\cong K\cong\mathbb Z_2, \qquad Z(SU(4)/K)\cong\mathbb Z_4/K\cong\mathbb Z_2.

Here the surviving center is generated by the class of iI4iI_4, and it acts nontrivially on the descended 66. A representation can descend without being trivial on the remaining center. To see that no extra center appears in this quotient, a central coset representative gg has commutators ghg−1h−1∈Kghg^{-1}h^{-1}\in K for all h∈SU(4)h\in SU(4); continuity and connectedness force that discrete-valued map to be the identity, so gg was already central.

Adding a fundamental 44 adds b=1b=1, leaving only the identity in the common kernel. The dimensions independently check as (42)=6\binom42=6 and 42−1=154^2-1=15. Enter rank N=4N=4 with labels 0,1,0;1,0,1 in matter-compatible quotients, then add 1,0,0.

4. The order of a product kernel is not enough

Section titled “4. The order of a product kernel is not enough”

In G~=SU(2)L×SU(2)R\widetilde G=SU(2)_L\times SU(2)_R, compare

ΓL=⟨(−I,I)⟩,Γdiag=⟨(−I,−I)⟩.\Gamma_L=\langle(-I,I)\rangle, \qquad \Gamma_{\mathrm{diag}}=\langle(-I,-I)\rangle.

Both are central subgroups of order 22. Does the representation (2,2)(\mathbf2,\mathbf2) descend through each? What about (2,1)(\mathbf2,\mathbf1)? Explain why the quotient fundamental group alone cannot decide this.

On VnL⊗VnRV_{n_L}\otimes V_{n_R} the two generators act as

ρ(−I,I)=(−1)nL,ρ(−I,−I)=(−1)nL+nR.\rho(-I,I)=(-1)^{n_L}, \qquad \rho(-I,-I)=(-1)^{n_L+n_R}.

The (2,2)(\mathbf2,\mathbf2) has (nL,nR)=(1,1)(n_L,n_R)=(1,1). It fails the first test and passes the second. The (2,1)(\mathbf2,\mathbf1) has (1,0)(1,0) and fails both. Thus including both multiplets obstructs either displayed order-22 quotient.

Each displayed quotient has fundamental group isomorphic to Z2\mathbb Z_2, since the covering product is simply connected. The abstract isomorphism type of the kernel loses its position inside the product center. Descent retains that embedding. The product gauge-group tool uses explicit center generators for this reason. For a descent check there, choose the two SU(2)SU(2) factors, zero matter charges under its required spectator U(1)U(1), and zero U(1)U(1) phase in the quotient generator. The spectator contributes an extra Z\mathbb Z to the tool’s fundamental group; that is not part of the two-factor problem above.

Use the two circle inclusions

U(1)→SU(2): z↦diag⁡(z,z−1),SO(2)→SO(3): R(φ)↦diag⁡(R(φ),1).U(1)\to SU(2):\ z\mapsto\operatorname{diag}(z,z^{-1}), \qquad SO(2)\to SO(3):\ R(\varphi)\mapsto\operatorname{diag}(R(\varphi),1).

Each source circle parameter has period 2π2\pi. Identify both cosets with S2S^2 and choose compatible sphere generators as in the topology lesson.

  1. Compute the image of a unit sphere winding under ∂:π2(G/H)→π1(H)\partial:\pi_2(G/H)\to\pi_1(H) in each case.
  2. How many principal SU(2)SU(2) and principal SO(3)SO(3) bundle classes exist on S2S^2?
  3. Can an odd SO(2)SO(2) clutching loop arise from a reduction on the sphere of a smooth SO(3)SO(3) bundle over a ball?

The SU(2)SU(2) circle loop is contractible in SU(2)SU(2); the SO(3)SO(3) circle loop of winding mm maps to m mod 2m\bmod2. Since both ambient groups have vanishing π2\pi_2, exactness gives boundary images Z\mathbb Z and 2Z2\mathbb Z, respectively. With the compatible sign convention,

∂SU(1)=1,∂SO(1)=2.\partial_{\mathrm{SU}}(1)=1, \qquad \partial_{\mathrm{SO}}(1)=2.

The spin cover maps the first circle to the second with degree 22 while identifying the orbit spheres, which checks this normalization. Nevertheless each orbit has π2(S2)=Z\pi_2(S^2)=\mathbb Z.

Principal bundles over S2S^2 instead use π2(BG)=π1(G)\pi_2(BG)=\pi_1(G) for connected GG. There is one SU(2)SU(2) bundle class and two SO(3)SO(3) bundle classes. An odd SO(2)SO(2) clutching loop induces the nontrivial SO(3)SO(3) class; it cannot extend over a ball, where every principal bundle is trivial. This is a topological obstruction under the smooth extension assumption, not a claim about a monopole solution’s energy or stability. Compare both cases in the topology workbench.

A proposed argument says: “The kernel of U(1)→U(1)U(1)\to U(1), z↦zkz\mapsto z^k, is Zk\mathbb Z_k, so the target has π1=Zk\pi_1=\mathbb Z_k.” Identify the error for k≥2k\geq2 and write the correct sequence.

The source circle is not simply connected. The map induces winding multiplication by kk, so the correct exact sequence is

0⟶Z→×kZ→ mod kZk⟶0.0\longrightarrow\mathbb Z\xrightarrow{\times k}\mathbb Z \xrightarrow{\bmod k}\mathbb Z_k\longrightarrow0.

The kernel records the quotient of the target fundamental group by the image of the source fundamental group. Only a universal covering removes the source term. See Conrad, Fundamental groups of Lie groups, pp. 1–2 and the topology formula reference.

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