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Depth-Zero Representation Inspector

Depth-Zero Representation Inspector

Enter a compact type, with optional discrete/tempered data and general-linear factors. Follow the construction and see how each sign selects the representation.

The result shows the packet-table symbol with its actual signs and the construction of that member. Use View depth-zero L-packet to return to its packet.

Reading the representation data​

In (2,[2],alpha,1,[1]), the first 2 is the degree, the second is the Jordan size, the next 1 is the Frobenius determinant tt, and the final [1] is the enhancement sign. This block has dimension 2⋅2=42\cdot2=4.

Enhancement signs are +1+1 or −1-1. A 0 in the final list means no sign coordinate. In the finite type, zero marks an absent factor or sign choice; indices and Jordan sizes can be 2 or larger.

Character subscripts give the field degree: α2\alpha_2 is a character of Fq2×\mathbb F_{q^2}^{\times}, and β6\beta_6 of Fq6×\mathbb F_{q^6}^{\times}. For U, degree dd gives subscript 2d2d. Enter alpha or beta without a suffix; the degree comes from the tuple. Exact input @k displays the exponent in brackets, as in θ2[10]\theta_2^{[10]}.

For a discrete series, the steps construct the supercuspidal representation, enlarge surviving blocks, and restore removed pairs. Each step shows the actual sizes, signs, and induction. Equal-sign pairs (+1,+1)(+1,+1) and (−1,−1)(-1,-1) can give the same induction; the common sign selects different subrepresentations. The Sp₈ example displays both choices and highlights the selected one.

Compact supercuspidal input​

The finite types on sides y,zy,z specify the compact induction σ=c ⁣-Ind⁡JG(F)Λ\sigma=\operatorname{c\!-Ind}_J^{G(F)}\Lambda, with lattice form By⊥ϖBzB_y\perp\varpi B_z. Their order and character signs matter.

For Sp, enter (a,b,u) for each side. Its quadratic finite cuspidal indices are a=m+a=m_+ and b=m−b=m_-, with rank contribution a(a+1)+b2a(a+1)+b^2. When b>0b>0, u=±1u=\pm1 specifies the actual finite character through the normalized transvection value. When b=0b=0, enter u=0. The other finite sign is determined by

vx=(−1)ax+bx+∑P⌈mx,P/2⌉.v_x=(-1)^{a_x+b_x+\sum_P\lceil m_{x,P}/2\rceil}.

For odd SO, enter (m_plus,m_minus,e0,e1) on both sides. Side yy is odd orthogonal; side zz is even orthogonal. The signs e0,e1e_0,e_1 retain the reflection action on the full stabilizer S(O(Vy)×O(Vz))\mathrm S(\mathrm O(V_y)\times\mathrm O(V_z)). Enter zero for a missing even-orthogonal index's sign. Simultaneously twisting both full orthogonal factors by determinant describes the same restriction; the app uses the representative e0,y=+1e_{0,y}=+1.

For unramified U, the staircase types suffice; there are no extra classical quadratic-index fields.

Enter finite staircase types as (d,theta,m_y,m_z). Here theta is an actual named self-dual orbit, or an exact @k orbit with numerical q. Its degree is even in Sp/SO and odd over WEW_E in U. Each connected finite Jordan factor has the cuspidal unitary staircase (m,m−1,…,1)(m,m-1,\ldots,1). Omit an orbit if both indices are zero. The group size and pure inner form are inferred from these data.

Leave the discrete/tempered and general-linear fields empty for a classical supercuspidal. For GL, enter the general-linear factors directly; a single factor (d,[1],theta,t,0) specifies the depth-zero supercuspidal with tame orbit theta and Frobenius determinant t.

Other depth-zero representations​

Enter optional discrete/tempered data as:

(d,[a₁,…],theta,t,[ε₁,…]).

These tuples have exponent zero. Their signs select the constituent; repeat the same sign for repeated sizes and use 0 for blocks with no sign coordinate. The app checks that reducing these blocks recovers the entered compact type, including its signs. Leave the field empty to use that type's supercuspidal parameter, or enter 0 for a trivial discrete core.

The general-linear factors use (d,[a₁,…],theta,t,s). For a classical group, require s>0s>0: the app adjoins the dual factors with exponent −s-s and forms the Langlands quotient. Zero-exponent factors belong in the discrete/tempered field. For GL, all real exponents are allowed.

The compact type supplies the actual supercuspidal base. On the cuspidal support of discrete series for pp-adic quasisplit Sp(N)\mathrm{Sp}(N) and SO(N)\mathrm{SO}(N), Bin Xu, Theorem 10.1 and §10, describes the admissible-triple reduction used here.

Whittaker normalization and q​

All signs use the fixed Whittaker normalization: upper integral pinning, Ψ\Psi trivial on ϖOF\varpi\mathcal O_F and nontrivial on OF\mathcal O_F, and the stated Gauss-sum and pure-inner-form conventions. Changing this normalization changes the sign labels, while preserving the ordinary parameter.

Leave q symbolic. The finite-type dictionary and packet labels require no numerical character evaluation. Numerical q is needed for exact @k character orbits and checks the large odd residue-field range: q>2Rq>2R for Sp and odd SO, and q≥nq\ge n for U. The mixed quadratic Sp/SO assignments assume the signed quadratic-twist comparison, in addition to the unsigned reducibility results of Lust–Stevens.

Examples​

The links below fill the representation fields and display its construction. They keep q symbolic unless a number is specified.