diff 56bc728..f6bf760 symmetric_tensor_categories_fiber_v2.txt
diff --git a/symmetric_tensor_categories_fiber_v2.txt b/symmetric_tensor_categories_fiber_v2.txt
index 77f55fc..2058a0b 100644
--- a/symmetric_tensor_categories_fiber_v2.txt
+++ b/symmetric_tensor_categories_fiber_v2.txt
@@ -60,7 +60,7 @@ every finite symmetric tensor category over an algebraically closed
 field k of characteristic p>0 admits a k-linear exact faithful
 strong symmetric monoidal functor to a finite higher Verlinde
 category Ver_{p^n}(k).  The result covers every prime, including
-p=2, and the height n may depend on mathcal C.calC.
+p=2, and the height n may depend on C.
 
 
 tableofcontents
@@ -78,7 +78,7 @@ p>0.
 [finite symmetric tensor category]
 
 A finite symmetric tensor category over k is a
-k-linear abelian rigid symmetric monoidal category mathcal CcalC
+k-linear abelian rigid symmetric monoidal category C
 such that:
 [label=(arabic*)]
  the tensor product is biexact;
@@ -95,14 +95,14 @@ Intuition: it is the ``linear algebra'' world where you can tensor
 and dualise, everything has finite length, and the unit behaves like
 the one-dimensional vector space.  The simplest example is
 Vec_k, the category of finite-dimensional k-vector spaces;
-when p>2 its partner is sVec_k, the mathbb Z/2-gradedbbZ/2-graded
+when p>2 its partner is sVec_k, the Z/2-gradedbbZ/2-graded
 version with the Koszul sign in the symmetry.
 
 [fiber functor]
-A fiber functor mathcal CcalCto mathcal DcalD between finite
+A fiber functor C D between finite
 symmetric tensor categories is a k-linear exact faithful strong
 symmetric monoidal functor.  ``Fiber functor'' in the classical
-sense is the special case mathcal DcalD = Vec_k; the target being a
+sense is the special case D = Vec_k; the target being a
 non-vector-space category is what forces the tower in positive
 characteristic.
 
@@ -134,7 +134,7 @@ in Benson--Etingof (2019).
 
 
 Intuition for Ver_p: it is the ``semisimplification'' of
-Rep_k(mathbb Z/p):bbZ/p): one kills every morphism f with tr(gf)=0
+Rep_k(Z/p):bbZ/p): one kills every morphism f with tr(gf)=0
 for all g; the simple objects correspond to Jordan blocks of
 lengths 1,...,p-1.  For p=2 this collapses to
 Vec_k; for p=3 it gives supervector spaces.  Each higher level
@@ -149,10 +149,10 @@ Here is the result we prove.
 
 For every prime p, every algebraically closed field k of
 characteristic p, and every finite symmetric tensor category
-mathcal CcalC over k, there exist an integer nge 1 and a fiber
+C over k, there exist an integer nge 1 and a fiber
 functor
 [
-  mathcal CcalC → Ver_{p^n}(k).
+  C → Ver_{p^n}(k).
 ]
 
 
@@ -166,15 +166,15 @@ implies the finite part of all the consequences we discuss.
 
 We iteratively apply a semilinear higher Frobenius functor Phi,
 each application adding one fresh Verlinde factor while forcing
-the original mathcal CcalC factor to shrink into its Frobenius-exact
+the original C factor to shrink into its Frobenius-exact
 subcategory.  After at most N iterations, where N is the number
-of simple objects of mathcal C,calC, all first components land in the
+of simple objects of C, all first components land in the
 Serre closure of that subcategory.  The essential ingredients are:
 
 [label=Step arabic*.,ref=step:arabic*]
  Restricted tilting modulo a Steinberg module.
         For every finite-dimensional module D over the
-        elementary abelian group E_r = (mathbb Z/p)^r,bbZ/p)^r, the
+        elementary abelian group E_r = (Z/p)^r,bbZ/p)^r, the
         tensor product St_{r-1} ⊗  D of a fixed Steinberg
         module with D is a restriction of an SL_2-tilting
         module.  This is the Coulembier--Flake conjecture; we prove
@@ -183,7 +183,7 @@ Serre closure of that subcategory.  The essential ingredients are:
         The previous step lets us define, for every embedding
         E_r↪ U(k)⊆ SL_2(k), a
         k-linear additive strong symmetric monoidal functor
-        Phi:mathcal CcalCto mathcal CcalCboxtimes Ver_{p^r}(k)
+        Phi:C C Ver_{p^r}(k)
         that is only semilinear (Phi(af) = a^{p^r}Phi(f)).
  Exactness by support.  For a well-chosen
         embedding of E_r (with r minimal), Phi is actually
@@ -195,7 +195,7 @@ Serre closure of that subcategory.  The essential ingredients are:
         constrains composition factors of Phi(S) for simple
         S.  Iterating Phi finitely many times pushes the
         first component into the Serre closure of the
-        Frobenius-exact tensor subcategory mathcal C_calC_{ex}.
+        Frobenius-exact tensor subcategory C_{ex}.
 
 
 After these four steps, a few more tasks finish the argument:
@@ -218,15 +218,15 @@ corollaries.
 The definition of finite symmetric tensor category was chosen so
 that the usual Tannakian toolkit applies.  We make this explicit.
 
-[mathcal CcalC is modules over a finite algebra]
+[C is modules over a finite algebra]
 
-Let mathcal CcalC be a finite symmetric tensor category.  Then the
+Let C be a finite symmetric tensor category.  Then the
 unit object is simple, and there is a projective generator
-Pinmathcal C.calC.  The functor omega = Hom_{mathcal C}calC(P,-) is
-exact and faithful, and mathcal CcalC is equivalent, as a k-linear
+PinC.  The functor omega = Hom_{C},-) is
+exact and faithful, and C is equivalent, as a k-linear
 abelian category, to the category of finite-dimensional modules
 over the finite-dimensional k-algebra
-A = End_{mathcal C}calC(P)^{op}.
+A = End_{C}{op}.
 
 
 Proof. 
@@ -236,7 +236,7 @@ Uto V ⊗  U coming from mathbf 1bf1twoheadrightarrow V has
 zero composite with the subobject V ⊗  Utwoheadrightarrow V.
 So V ⊗  U=0.  Put W=ker(mathbf 1bf1to U^*).  Then W
 sits inside a short exact sequence with U, V, and tensoring by
-W gives Wsimeq V.  The endomorphism ring of the unit has no
+W gives W~= V.  The endomorphism ring of the unit has no
 idempotents, so V=0.
 
 For the projective generator: pick surjections Q_ito S_i from
@@ -244,7 +244,7 @@ projectives onto the finitely many simples; set
 P=⊕_i Q_i.  Projectivity lifts surjections to P, so
 every object is a quotient of P^{ ⊕  m} for some m.  Exact
 faithfulness comes from lifting along Pto image.  To identify
-mathcal CcalCsimeq A-mod, note that presenting objects by
+C~= A-mod, note that presenting objects by
 copies of P and using projectivity is fully faithful on the level
 of presentations, and every finite A-module has a finite free
 presentation.
@@ -256,22 +256,22 @@ simples.
 
 ## Deligne products
 
-For finite k-linear abelian categories mathcal A,calA,mathcal B,calB, the
-Deligne product mathcal AcalAboxtimesmathcal BcalB is the
+For finite k-linear abelian categories A,B, the
+Deligne product A BcalB is the
 universal recipient of functors that are k-bilinear and right
-exact in each variable.  When mathcal AcalAsimeq A-mod and
-mathcal BcalBsimeq B-mod, we have
-mathcal AcalAboxtimesmathcal BcalBsimeq (A ⊗ _k B)-mod,
+exact in each variable.  When A~= A-mod and
+B~= B-mod, we have
+A BcalB~= (A ⊗ _k B)-mod,
 and its simple objects are the exterior products of the simples of
 the two factors (here we use k algebraically closed).
 
 [combining exact tensor functors]
 
-Let mathcal A_1,...,calA_1,...,mathcal A_s,calA_s,mathcal ZcalZ be finite
-symmetric tensor categories and let F_i:mathcal A_icalA_itomathcal ZcalZ
+Let A_1,...,calA_1,...,A_s,Z be finite
+symmetric tensor categories and let F_i:A_i ZcalZ
 be exact k-linear strong symmetric monoidal functors.  Then
 [
-  H:mathcal A_1calA_1boxtimes...boxtimesmathcal A_scalA_stomathcal Z,calZ,
+  H:A_1 A_scalA_stoZ,
   
   H(X_1boxtimes...boxtimes X_s)
    = F_1(X_1) ⊗ ... ⊗  F_s(X_s),
@@ -283,7 +283,7 @@ functor.
 Proof. 
 The displayed multilinear functor has a right-exact extension by
 the universal property of the Deligne product.  Symmetry in
-mathcal ZcalZ gives the tensor constraint by rearranging factors, and
+Z gives the tensor constraint by rearranging factors, and
 coherence extends by the same universal property.  The result
 preserves duals.  A short exact sequence dualises, is sent to a
 right-exact sequence, and is dualised back; hence the functor is
@@ -292,24 +292,24 @@ also left exact.
 
 ## Frobenius--Perron dimension
 
-For finite tensor categories the Grothendieck ring K_0(mathcal C)calC)
+For finite tensor categories the Grothendieck ring K_0(C)
 is finitely freely generated by simple classes.  Symmetry makes it a
 commutative ring, and the Frobenius--Perron theorem identifies a
 unique positive normalised real character
-d = FPdim : K_0(mathcal C)calC)tomathbb RbbR with d(mathbf 1)=1bf1)=1
+d = FPdim : K_0(C) RbbR with d(mathbf 1)=1bf1)=1
 and d multiplicative on classes.  Key facts, all in Etingof--
 Gelaki--Nikshych--Ostrik (2015):
 
 [FP dimension toolkit]
 
-Let mathcal CcalC be a finite tensor category.
+Let C be a finite tensor category.
 [label=(roman*)]
  d(X)ge 1 for every nonzero X; equality if and only if
         X is invertible.
  If 0to Xto Yto Zto 0 is exact, then
         d(Y)=d(X)+d(Z).
  On a Deligne product, d(Aboxtimes B)=d(A),d(B).
- If F:mathcal CcalCtomathcal DcalD is an exact strong monoidal
+ If F:C DcalD is an exact strong monoidal
         functor of finite tensor categories, then
         d(F(X))=d(X) for every X.
 
@@ -328,10 +328,10 @@ mod-p congruence.
 
 ## The statement
 
-Let G = SL_2(k), and let Usimeqmathbb G_abbG_a be its upper
+Let G = SL_2(k), and let U~=G_a be its upper
 unipotent subgroup, identified with k via
 u(t) = (1&t0&1).
-For rge 1 put E_r = (mathbb Z/p)^rbbZ/p)^r and let
+For rge 1 put E_r = (Z/p)^rbbZ/p)^r and let
 iota:E_r↪ U(k) be any injective homomorphism.
 Write R = R_iota for the restriction of G-modules along iota.
 
@@ -346,11 +346,11 @@ weight a.
 
 [restricted-tilting theorem]
 
-Let rge 1, E_r = (mathbb Z/p)^r,bbZ/p)^r, and iota:E_rto U(k) any
+Let rge 1, E_r = (Z/p)^r,bbZ/p)^r, and iota:E_rto U(k) any
 injective homomorphism.  For every finite-dimensional kE_r-module
 D there is a tilting G-module T such that
 [
-  R_iota(St_{r-1}) ⊗  D cong R_iota(T)
+  R_iota(St_{r-1}) ⊗  D ~= R_iota(T)
 ]
 as kE_r-modules.
 
@@ -366,7 +366,7 @@ We do three things:
         U-module widehatwidehat DD of bounded ``degree'' (a bound on
         polynomial degree of the unipotent action matrix);
  use widehatwidehat DD to construct a G-equivariant vector
-        bundle mathcal McalM on the plane mathbb A^2_kbbA^2_k whose
+        bundle M on the plane A^2_k whose
         origin fibre has all simple composition factors below a
         height bound;
  tensor by St_{r-1}, observe the resulting bundle's
@@ -386,7 +386,7 @@ matrix rho_D(u(t)); this does not depend on a chosen basis.
 
 For every finite-dimensional kE_r-module D, there is a
 finite-dimensional rational U-module widehatwidehat DD of degree < p^r
-such that widehatwidehat D|_D|_{E_r}cong D along iota.
+such that widehatwidehat D|_D|_{E_r}~= D along iota.
 
 
 Proof. 
@@ -395,23 +395,23 @@ vector space
 C_q = span_k{1,t,...,t^{q-1}}⊆ k[t]
 (with q=p^r) is a subcoalgebra of k[t] with
 Delta f(t,s) = f(t+s).  Evaluation at H gives a coalgebra map
-ev_H : C_q to k^H = mathcal O(E_r),calO(E_r), which is a
+ev_H : C_q to k^H = O(E_r), which is a
 bijection: the two sides have dimension q, and a degree-<q
 polynomial vanishing at the q distinct points of H is zero.
-Transporting the mathcal O(E_r)-coactioncalO(E_r)-coaction defining D across
+Transporting the O(E_r)-coactioncalO(E_r)-coaction defining D across
 ev_H, then including C_q subset k[t], gives a
 rational U-module of degree <q.  Its restriction is D.
 
 
 ## The G-equivariant bundle on the plane
 
-Now consider the orbit map pi : Gtomathbb A^2∖bbA^2∖{0},
-gmapsto g e_1, with e_1=(1,0).  This is a right U-torsor:
+Now consider the orbit map pi : GtoA^2∖bbA^2∖{0},
+g|-> g e_1, with e_1=(1,0).  This is a right U-torsor:
 the fibres are right U-cosets and on the standard opens xne 0,
 yne 0 it has obvious rational sections.  Form the associated
 vector bundle
 [
-  mathcal EcalE = Gtimes^U widehatwidehat D,D,
+  E = Gtimes^U widehatwidehat D,D,
    (g,d)sim(gu,u^{-1}d),
 ]
 on the punctured plane, with G acting by left multiplication.
@@ -419,27 +419,27 @@ The fibre at e_1 is widehatwidehat DD itself.
 
 [extension and weight bound]
 
-The bundle mathcal EcalE extends to a G-equivariant vector bundle
-mathcal McalM on the whole affine plane, and every simple
+The bundle E extends to a G-equivariant vector bundle
+M on the whole affine plane, and every simple
 composition factor of the origin fibre
-M_0 = mathcal M|_0calM|_0 has highest weight < q.
+M_0 = M|_0calM|_0 has highest weight < q.
 
 
 Proof. 
-Extension.  A coherent extension mathcal FcalF exists on the
-noetherian affine plane.  Its double dual mathcal McalM = mathcal
-F^calF^{**} is a coherent reflexive sheaf restricting to mathcal E.calE.
-On the regular surface mathbb A^2bbA^2 every reflexive coherent sheaf
+Extension.  A coherent extension F exists on the
+noetherian affine plane.  Its double dual M = mathcal
+F^calF^{**} is a coherent reflexive sheaf restricting to E.
+On the regular surface A^2 every reflexive coherent sheaf
 is locally free: at a closed point the stalk has depth two, so the
 Auslander--Buchsbaum formula gives projective dimension zero, and at
 the generic point and at the generic point of a curve the stalks are
-trivially free.  Hence mathcal McalM is a vector bundle.
+trivially free.  Hence M is a vector bundle.
 
 Equivariance.  Over the punctured plane we have a
 G-equivariant bundle isomorphism
-pi_2^*mathcal McalMcong a^*mathcal McalM for the action
-a:Gtimesmathbb A^2bbA^2tomathbb A^2bbA^2 and projection
-pi_2:Gtimesmathbb A^2bbA^2tomathbb A^2.bbA^2.  Both sides are locally
+pi_2^*M a^*M for the action
+a:GtimesA^2 A^2bbA^2 and projection
+pi_2:GtimesA^2 A^2.bbA^2.  Both sides are locally
 free, so the Hom-sheaf is locally free and its sections extend
 across the codimension-two subset Gtimes{0}; the extensions of
 the isomorphism and its inverse remain inverse because the two
@@ -453,7 +453,7 @@ h_a = diag(a,a^{-1}); the bundle action of h_a gives
 a linear identification of fibres at e_1 and at ae_1, and
 h_a^{-1}u(t)h_a = u(a^{-2}t).  Hence on every nonzero fibre over
 ell the U-action has degree <q.  Let
-A = Gamma(ell,mathcal EcalE nd(mathcal M|_calM|_ell)) and write the
+A = Gamma(ell,E nd(M|_calM|_ell)) and write the
 U-action as an element of A ⊗ _k k[t],
 sum_j b_j t^j.  For jge q, b_j vanishes on every nonzero
 fibre, so b_j = 0 (since k is infinite and A is torsion-free
@@ -477,7 +477,7 @@ p=2:
 
   L(a) = T(a)(0le a<p),
   
-  T(a) ⊗  T(b)^{(1)}simeq T(a+pb)
+  T(a) ⊗  T(b)^{(1)}~= T(a+pb)
   (p-1le ale 2p-2, bge 0),
 
 where (1) means pullback along the Frobenius.  See Benson--
@@ -499,7 +499,7 @@ tilting by (eq:sl2-tilting-basics).
 For m>1, write h = d + p h' with 0le d<p and h'<p^{m-1}.
 Steinberg's tensor product theorem gives
 [
-  St_{m-1} ⊗  L(h) cong
+  St_{m-1} ⊗  L(h) ~=
   L(d) ⊗  St_1 ⊗ 
   (St_{m-2} ⊗  L(h'))^{(1)}.
 ]
@@ -518,25 +518,25 @@ M|_0,calM|_0, we have:
 
 is a tilting G-module.  The remaining step is to compare T
 (the origin fibre of
-mathcal NcalN = St_{r-1} ⊗ _k mathcal M)calM) with the e_1-fibre
-of mathcal N.calN.
+N = St_{r-1} ⊗ _k M) with the e_1-fibre
+of N.
 
 ## Formal comparison of fibres
 
 [comparison with a tilting origin fibre]
 
-Let mathcal NcalN be a G-equivariant vector bundle on mathbb A^2bbA^2
-whose origin fibre T = mathcal N|_0calN|_0 is tilting.  Then
-mathcal N|_calN|_{e_1}cong T|_U as rational U-modules.
+Let N be a G-equivariant vector bundle on A^2
+whose origin fibre T = N|_0calN|_0 is tilting.  Then
+N|_calN|_{e_1}~= T|_U as rational U-modules.
 
 
 Proof. 
 Jet trivialisation.  Let A=k[x,y], mathfrak m=(x,y),frakm=(x,y),
-and N=Gamma(mathbb A^2,bbA^2,mathcal N),calN), a possibly
+and N=Gamma(A^2,N), a possibly
 infinite-dimensional rational G-module.  Local freeness gives
 canonical G-isomorphisms
 
-  mathfrak m^jfrakm^j N/mathfrak m^frakm^{j+1}N cong
+  mathfrak m^jfrakm^j N/mathfrak m^frakm^{j+1}N ~=
   Sym^j(V^*) ⊗ _k T.
 
 The target has a good filtration.  Tensor products of Sym's of
@@ -564,15 +564,15 @@ k[[x,y]] ⊗ _k Txrightarrow{sim}widehatwidehat N.N.
 
 Fibre comparison.  Restrict to the fixed line y=0, pass
 to K = k((x)): this gives a U_K-isomorphism
-varphi:T_Kcong mathcal N_calN_{xe_1}.  To cancel the parameter
+phi:T_Kcong N_{xe_1}.  To cancel the parameter
 mismatch we use the torus element h = diag(x,x^{-1}):
 since hu(t)h^{-1} = u(x^2 t), the composite
-f = b_h^{-1}varphirho_T(h) intertwines the original
-U-actions (where b_h : mathcal N_calN_{e_1}tomathcal N_calN_{xe_1} is
+f = b_h^{-1}phirho_T(h) intertwines the original
+U-actions (where b_h : N_{e_1}toN_{xe_1} is
 bundle transport).
 
 Descent to k.  The space
-L = Hom_U(T,mathcal N_calN_{e_1}) is cut out by finitely many
+L = Hom_U(T,N_{e_1}) is cut out by finitely many
 k-linear equations in fixed k-bases, so L_K = L ⊗ _k K.
 The determinant on L is nonzero over K (witnessed by f), so
 nonvanishing at some k-point (since k is infinite) gives the
@@ -580,16 +580,16 @@ required isomorphism over k.
 
 
 Proof. [Proof of cref{thm:restricted-tilting}]
-Apply cref{prop:extension-bound} to get mathcal McalM with origin
+Apply cref{prop:extension-bound} to get M with origin
 fibre M_0 whose simple factors have highest weight <q=p^r.
 By cref{lem:steinberg-tilting}, T = St_{r-1} ⊗  M_0 is
 tilting.  Apply cref{lem:formal-comparison} to
-mathcal NcalN = St_{r-1} ⊗ _kmathcal M:calM: its origin fibre is
+N = St_{r-1} ⊗ _kM:calM: its origin fibre is
 T, so
 [
-  mathcal N|_calN|_{e_1} cong T|_U.
+  N|_calN|_{e_1} ~= T|_U.
 ]
-But by construction mathcal N|_calN|_{e_1} restricts to
+But by construction N|_calN|_{e_1} restricts to
 R(St_{r-1}) ⊗  D along E_r↪ U(k), hence so
 does T.  Set T_{out} := T; the theorem follows.
 
@@ -603,20 +603,20 @@ does T.  Set T_{out} := T; the theorem follows.
 
 Fix rge 1, q=p^r, and an embedding
 E = E_r ↪ U(k).  We write R for restriction of
-SL_2-modules along this embedding, and mathcal WcalW = Ver_{p^r}(k).
-Let mathcal T⊆calT⊆ Rep_k(SL_2) be the category of tilting
+SL_2-modules along this embedding, and W = Ver_{p^r}(k).
+Let T⊆calT⊆ Rep_k(SL_2) be the category of tilting
 modules, and let I_r be the tensor ideal generated by
 St_r = L(p^r-1).
 
 Concretely, I_r is defined by demanding that T(a) (the
 indecomposable tilting module of highest weight a) vanish in
-mathcal T/I_rcalT/I_r whenever age p^r - 1; this is the standing
+T/I_rcalT/I_r whenever age p^r - 1; this is the standing
 convention in this circle of papers.
 
-The functor mathcal T/I_rcalT/I_rtomathcal WcalW is an equivalence onto a
+The functor T/I_rcalT/I_rtoW is an equivalence onto a
 full subcategory (Benson--Etingof--Ostrik (2023), Theorem 4.2(i)).
 Stable restriction gives a faithful quotient functor
-mathcal T/I_rcalT/I_rtoStab(E) :=
+T/I_rcalT/I_rtoStab(E) :=
 Rep_k(E)/(projectives).
 
 Coulembier--Flake (2026, Theorem 5.4.3) state: if for every
@@ -624,9 +624,9 @@ finite-dimensional E-module D the tensor R(St_{r-1) ⊗  D
 is a restriction of a tilting, then there is a k-linear strong
 symmetric monoidal functor}
 
-  Θ : Rep_k(E)→ mathcal WcalW
+  Θ : Rep_k(E)→ W
   quadwithquad
-  Θ(R(T)) simeq Σ_r(Tbmod I_r).
+  Θ(R(T)) ~= Σ_r(Tbmod I_r).
 
 The hypothesis is exactly cref{thm:restricted-tilting}.  So
 cref{thm:restricted-tilting} produces Θ, once and for all
@@ -654,7 +654,7 @@ is the free module, so Θ kills every projective.  When
 H<E is proper, St_{r-1}in I_s at the level s =
 rank(H) so Res^E_H R(St_{r-1}) is projective; the tensor
 identity
-S ⊗ Ind_H^E D cong Ind_H^E(Res_H^E S ⊗  D) therefore
+S ⊗ Ind_H^E D ~= Ind_H^E(Res_H^E S ⊗  D) therefore
 gives a projective E-module, on which Θ vanishes.  Since
 Θ(S)ne0 and tensoring by a nonzero object is faithful,
 Θ(Ind_H^E D)=0.
@@ -662,26 +662,26 @@ gives a projective E-module, on which Θ vanishes.  Since
 
 ## Internal evaluation
 
-Let mathcal CcalC be a finite symmetric tensor category with
-projective generator P_0.  Write A = End_{mathcal C}calC(P_0)^{op},
-so mathcal CcalCsimeq A-mod.  An object of
-mathcal CcalCboxtimesRep_k(E) is an object of mathcal CcalC
+Let C be a finite symmetric tensor category with
+projective generator P_0.  Write A = End_{C}{op},
+so C~= A-mod.  An object of
+C is an object of C
 equipped with a commuting E-action.  Applying Θ to the
 underlying E-module and to the action maps produces an A-module
-object in mathcal W,calW, hence an object of
-mathcal CcalCboxtimesmathcal W.calW.  This is the internal
-extension Θ_{mathcal C}calC of Θ (Coulembier--Flake
+object in W, hence an object of
+C W.calW.  This is the internal
+extension Θ_{C} of Θ (Coulembier--Flake
 2026, Example 3.2.4 and Proposition 3.2.6; requires only
 additivity of Θ, not exactness).
 
 [evaluation at projectives]
 
-For Qinmathcal CcalC projective and Z an E-object of
-mathcal C,calC,
+For QinC projective and Z an E-object of
+C,
 [
- (Hom_{mathcal C}calC(Q,-)boxtimesId_mathcal W)calW)
-   (Θ_{mathcal C}calC(Z))
- cong Θ(Hom_{mathcal C}calC(Q,Z)).
+ (Hom_{C},-)boxtimesId_W)
+   (Θ_{C}
+ ~= Θ(Hom_{C},Z)).
 ]
 
 
@@ -698,21 +698,21 @@ Hom_A(Q,-).
 Give X^{ ⊗  q} the E-action coming from regular permutation
 of tensor positions.  Define
 
-  Phi(X) = Θ_{mathcal C}calC(X^{ ⊗  q})
-        in mathcal CcalCboxtimes mathcal W.calW.
+  Phi(X) = Θ_{C}{ ⊗  q})
+        in C W.
 
 
 [monoidal structure and semilinearity]
 
 Phi is additive, strong symmetric monoidal, strong k-linear
-after twisting scalars by Frobenius amapsto a^q, and satisfies
+after twisting scalars by Frobenius a|-> a^q, and satisfies
 Phi(af) = a^qPhi(f) for scalars ain k.
 
 
 Proof. 
 The monoidal constraint is the E-equivariant reordering
 [
-  (X ⊗  Y)^{ ⊗  q}cong X^{ ⊗  q} ⊗  Y^{ ⊗  q}
+  (X ⊗  Y)^{ ⊗  q}~= X^{ ⊗  q} ⊗  Y^{ ⊗  q}
 ]
 with the diagonal action on the right, applied through the internal
 monoidal extension of Coulembier--hspace{0pt}Flake (2026, Section 3.3.2).
@@ -727,8 +727,8 @@ calculation on scalars.
 
 Combining cref{eq:phi} and cref{lem:projective-evaluation}:
 
- (Hom_{mathcal C}calC(Q,-)boxtimesId_mathcal W)(calW)(Phi(X))
- cong Θ(Hom_{mathcal C}calC(Q,X^{ ⊗  q}))
+ (Hom_{C},-)boxtimesId_W)(
+ ~= Θ(Hom_{C},X^{ ⊗  q}))
 
 for every projective Q.
 
@@ -736,14 +736,14 @@ for every projective Q.
 
 [Phi exact iff image nonzero]
 
-If there are projective objects P,Qinmathcal CcalC with
-Θ(Hom_{mathcal C}calC(Q,P^{ ⊗  q}))ne0, then Phi is
+If there are projective objects P,QinC with
+Θ(Hom_{C},P^{ ⊗  q}))ne0, then Phi is
 exact.
 
 
 Proof. 
 Cref{eq:phi-evaluation} gives Phi(P)ne0.  For a short exact
-sequence in mathcal C,calC, tensoring by P splits it because tensor
+sequence in C, tensoring by P splits it because tensor
 products of projectives with arbitrary objects are projective.
 The additive Phi preserves this split sequence.  Monoidality
 identifies the result as the original image sequence tensored by
@@ -758,7 +758,7 @@ and reflects exactness; the image sequence is exact.
 
 Now we need to actually find r and iota for which the criterion
 of cref{prop:phi-exactness} fires.  The strategy: take r minimal
-so that M(r) := Hom_{mathcal C}calC(P,P^{ ⊗  p^r}) (as a
+so that M(r) := Hom_{C},P^{ ⊗  p^r}) (as a
 kE_r-module via the regular permutation of tensor slots) is
 nonprojective; and then choose the embedding iota so that
 R(St_{r-1}) ⊗  M(r) stays nonprojective.
@@ -782,11 +782,11 @@ The group ring kH is local self-injective: its only simple is k
 with trivial action; its socle is generated by N_H=sum_{hin H}h;
 the augmentation ideal is nilpotent (induct on |H|, use a central
 order-p element z with (z-1)^p=0, descend to k[H/<
-z>]); and a nondegenerate pairing abmapsto coefficient of
+z>]); and a nondegenerate pairing ab|-> coefficient of
 1 identifies kH with its linear dual as a module.
 
 For kH-free modules, the norm map is an iso.  Converse: if
-N_Hmne0, the map kHto M, amapsto am is injective and splits
+N_Hmne0, the map kHto M, a|-> am is injective and splits
 by self-injectivity, so M has a free summand.  Strip off all free
 summands, leaving M' with N_HM'=0; if M'ne0 then N_H=M'_H=0
 by Nakayama, contradiction with an iso.  So M'=0.
@@ -798,17 +798,17 @@ implies the total norm iso (same argument).
 
 [independent actions multiply]
 
-Let finite p-groups H_i act on objects X_iinmathcal CcalC
+Let finite p-groups H_i act on objects X_iinC
 (i=1,...,s).  If omega(X_i) is projective over kH_i for
-exact faithful omega = Hom_{mathcal C}calC(P,-), then
+exact faithful omega = Hom_{C},-), then
 omega(X_1 ⊗ ... ⊗  X_s) is projective over
 k[H_1times...times H_s] (independent actions), and over every
 subgroup thereof.
 
 
 Proof. 
-Categorically, (X ⊗  Y)_{Htimes K}cong X_H ⊗  Y_K and
-(X ⊗  Y)^{Htimes K}cong X^H ⊗  Y^K
+Categorically, (X ⊗  Y)_{Htimes K}~= X_H ⊗  Y_K and
+(X ⊗  Y)^{Htimes K}~= X^H ⊗  Y^K
 (take kernels/cokernels one group at a time).  So
 nu_{Htimes K}(X ⊗  Y) = nu_H(X) ⊗ nu_K(Y).  If each
 nu_{H_i}(X_i) is iso, so is the product norm.  Applying exact
@@ -819,7 +819,7 @@ kH for any finite group, so projectivity is preserved.
 
 ## Existence of a minimal r
 
-Let E_a=(mathbb Z/p)^abbZ/p)^a act on p^a positions by its regular
+Let E_a=(Z/p)^abbZ/p)^a act on p^a positions by its regular
 representation; this induces an E_a-action on P^{ ⊗  p^a}.
 Set M(a) = omega(P^{ ⊗  p^a}), an E_a-module.
 
@@ -854,7 +854,7 @@ b_d = sum_{sigmainmathfrak S_d}frakS_dsigma acts nontrivially on
 P^{ ⊗  d}.
 
 On the other hand the action map
-kmathfrak S_dfrakS_dtoEnd_{mathcal C}calC(P^{ ⊗  d}) cannot be
+kmathfrak S_dfrakS_dtoEnd_{C}{ ⊗  d}) cannot be
 injective: length grows exponentially in d (bounded by
 ell(P)b^{d-1} with b=max_iell(S_i ⊗  P)) and the
 dimension of Hom(X,Y) is bounded by ell(X)ell(Y), whereas
@@ -879,9 +879,9 @@ mathfrak mfrakm = (g_i-1)_i.  The projectivised rank variety of
 a finite-dimensional module D is
 [
  supp(D) =
-  bigl{[alpha]inmathbb P^bbP^{r-1}(k) :
+  bigl{[alpha]inP^{r-1}(k) :
    D  not free over  k[t]/(t^p),
-    tmapstotextstylesum_ialpha_i(g_i-1)
+    t|->textstylesum_ialpha_i(g_i-1)
   bigr}.
 ]
 Two standard facts (Benson 2017; Coulembier--Flake 2025):
@@ -895,18 +895,18 @@ Two standard facts (Benson 2017; Coulembier--Flake 2025):
 
 If M is a nonprojective kE_r-module with all restrictions to
 proper subgroups projective, then every [alpha]insupp(M) has
-mathbb F_p-linearlybbF_p-linearly independent coordinates.
+F_p-linearlybbF_p-linearly independent coordinates.
 
 
 Proof. 
-For cin(mathbb F_p^r)^bbF_p^r)^ast, let H=ker c and
+For cin(F_p^r)^, let H=ker c and
 N = Ind_H^{E_r}k, the regular representation of E_r/Hcong
-mathbb Z/pbbZ/p (identified with k[z]/(z^p), generator acts by
+Z/pbbZ/p (identified with k[z]/(z^p), generator acts by
 1+z).  The element sum_ialpha_i(g_i-1) acts on N by
 h_alpha(z) = sum_ialpha_i((1+z)^{c_i}-1), whose linear
 coefficient is sum_i c_ialpha_i.
 
-If sum_i c_ialpha_ine0, then tmapsto h_alpha(z) is an iso
+If sum_i c_ialpha_ine0, then t|-> h_alpha(z) is an iso
 of truncated polynomial algebras, so N is free as k[t]/(t^p);
 if sum_i c_ialpha_i=0, then h_alphain(z^2), so
 h_alpha^{p-1}=0, incompatible with a free module of dimension
@@ -917,15 +917,15 @@ supp(N) = {[alpha] : sum_i c_ialpha_i=0}.  The tensor
 identity gives M ⊗ Ind_H^{E_r}kcongInd_H^{E_r}(M|_H), which
 is projective, so supp(M)capsupp(N)=∅.  Hence
 sum_i c_ialpha_ine0 for every nonzero c.  In particular the
-coordinates of every [alpha]insupp(M) are mathbb F_p-linearlybbF_p-linearly
+coordinates of every [alpha]insupp(M) are F_p-linearlybbF_p-linearly
 independent.
 
 
 [Steinberg support in coordinates]
 
-Let lambda_1,...,lambda_rin k be mathbb F_p-linearlybbF_p-linearly
+Let lambda_1,...,lambda_rin k be F_p-linearlybbF_p-linearly
 independent and define iota_lambda : E_rto SL_2(k),
-g_imapsto u(lambda_i).  Write R_lambda for restriction.  Then
+g_i|-> u(lambda_i).  Write R_lambda for restriction.  Then
 
  supp(R_lambda(St_{r-1})) =
  {[alpha] : sum_ialpha_ilambda_i^{p^j}=0
@@ -942,20 +942,20 @@ argument of cref{lem:support-independent}, the resulting
 p-dimensional module is free iff the coefficient is nonzero.
 
 Frobenius twist replaces lambda_i by lambda_i^{p^j}.
-Since St_{r-1}cong⊗_{j=0}^{r-2}St_1^{(j)}, the tensor
+Since St_{r-1}~=⊗_{j=0}^{r-2}St_1^{(j)}, the tensor
 product formula (eq:support-properties) gives an intersection
 of hyperplanes
 M_j : sum_ialpha_ilambda_i^{p^j}=0, exactly cref{eq:steinberg-support}.
 For r=1 the system is empty and St_0=k has
-supp(St_0)=mathbb P^0(k),bbP^0(k), consistent.
+supp(St_0)=P^0(k), consistent.
 
 
 ## Moore's lemma: choosing lambda
 
 [lambda solving prescribed equations]
 
-Let alpha_1,...,alpha_rin k be mathbb F_p-linearlybbF_p-linearly
-independent.  Then there exist mathbb F_p-linearlybbF_p-linearly independent
+Let alpha_1,...,alpha_rin k be F_p-linearlybbF_p-linearly
+independent.  Then there exist F_p-linearlybbF_p-linearly independent
 lambda_1,...,lambda_rin k with
 
  sum_ialpha_ilambda_i^{p^j} = 0,
@@ -975,16 +975,16 @@ additive polynomial f(X)=sum_{s=0}^{r-2}a_s X^{p^s} vanishes on
 the p^r-element span of the beta_i, but deg fle p^{r-2}, so
 f=0.
 
-Row space of B contains no nonzero mathbb F_p^r-vector:bbF_p^r-vector: if
-c_i = f(beta_i)inmathbb F_p,bbF_p, then the polynomial f^p-f
+Row space of B contains no nonzero F_p^r-vector:bbF_p^r-vector: if
+c_i = f(beta_i)inF_p, then the polynomial f^p-f
 vanishes on the same p^r-element set and has degree
 le p^{r-1}; so f^p-f=0, forcing f=0 (since deg f<p^{r-1}
 and f has zero constant term).
 
 Choose lambdainker B nonzero.  Kernel is one-dimensional.  Any
-cinmathbb F_p^rbbF_p^r with sum_i c_ilambda_i=0 belongs to the
+cinF_p^r with sum_i c_ilambda_i=0 belongs to the
 annihilator of ker B, i.e., to the row space of B, hence is
-c=0.  So lambda_i are mathbb F_p-linearlybbF_p-linearly independent.
+c=0.  So lambda_i are F_p-linearlybbF_p-linearly independent.
 Reading rows of B in reverse order, (alpha_i^{p^{-j}})_i, and
 raising the equations sum_ilambda_i^{p^s}alpha_i^{p^{-(r-2)}p^s}
 =0 to the p^{r-2}-th power gives (eq:moore).
@@ -999,7 +999,7 @@ R_lambda(St_{r-1}) ⊗  M nonprojective.
 
 
 Proof. 
-Pick [alpha]insupp(M); coordinates are mathbb F_p-linearlybbF_p-linearly
+Pick [alpha]insupp(M); coordinates are F_p-linearlybbF_p-linearly
 independent by cref{lem:support-independent}.  Choose lambda by
 cref{lem:moore-selection}; cref{lem:steinberg-support} then gives
 [alpha]insupp(R_lambda(St_{r-1})).  So the tensor product
@@ -1011,15 +1011,15 @@ R_lambda(St_{r-1}) ⊗  M is nonprojective.
 
 [exact higher Frobenius functor]
 
-Let mathcal CcalC be a finite symmetric tensor category over k of
+Let C be a finite symmetric tensor category over k of
 characteristic p>0.  Then there exist rge1 and an embedding
 E_r↪ U(k) such that the construction of
 cref{sec:higher} gives an exact additive strong symmetric monoidal
 functor
 [
- Phi:mathcal CcalCtomathcal CcalCboxtimesVer_{p^r}(k)
+ Phi:C CcalCboxtimesVer_{p^r}(k)
 ]
-with Phi(X)=Θ_{mathcal C}calC(X^{ ⊗  p^r}) and
+with Phi(X)=Θ_{C}{ ⊗  p^r}) and
 Phi(af)=a^{p^r}Phi(f).  Moreover, for every projective Q the
 evaluation (eq:phi-evaluation) holds.
 
@@ -1027,7 +1027,7 @@ evaluation (eq:phi-evaluation) holds.
 Proof. 
 Let P be the projective generator and r the minimal integer of
 cref{prop:first-nonprojective}.  Then
-M = Hom_{mathcal C}calC(P,P^{ ⊗  p^r}) is nonprojective with
+M = Hom_{C},P^{ ⊗  p^r}) is nonprojective with
 projective restriction to every proper subgroup of E_r.
 By cref{prop:support-selection} pick lambda so that
 R_lambda(St_{r-1}) ⊗  M is nonprojective.
@@ -1036,7 +1036,7 @@ R_lambda(St_{r-1}) ⊗  Mcong R_lambda(T) for a tilting
 module T.  By cref{lem:theta-detection},
 [
  0 ne Θ(R_lambda(T))
- cong Θ(R_lambda(St_{r-1})) ⊗ Θ(M).
+ ~= Θ(R_lambda(St_{r-1})) ⊗ Θ(M).
 ]
 So Θ(M)ne0.  Cref{prop:phi-exactness} with P=Q shows
 Phi is exact.
@@ -1047,14 +1047,14 @@ Phi is exact.
 
 % =================================================================
 
-We now have an exact Phi:mathcal CcalCtomathcal CcalCboxtimesmathcal
-W,calW, q=p^r, mathcal W=calW=Ver_{p^r}(k), semilinear.
+We now have an exact Phi:C CcalCboxtimesmathcal
+W,calW, q=p^r, W={p^r}(k), semilinear.
 Its image closes up on the first factor to the Serre closure of a
 Frobenius-exact subcategory.
 
 ## Ordinary Frobenius and a mod-p identity
 
-For Yinmathcal C,calC, let c be the cyclic permutation of the p
+For YinC, let c be the cyclic permutation of the p
 factors of Y^{ ⊗  p} and D = 1-c (so D^p=0).  Define the
 Etingof--Ostrik components:
 [
@@ -1065,12 +1065,12 @@ Etingof--Ostrik components:
 If ell_iinVer_p(k) is the simple object represented by a
 Jordan block of length i, then
 F(Y)=⊕_{i=1}^{p-1}F_i(Y)boxtimesell_i.  In the
-semilinear convention, the F_i(Y) are objects of mathcal CcalC
+semilinear convention, the F_i(Y) are objects of C
 itself.  F is not assumed exact.
 
 [mod-p identity in K_0]
 
-In K_0(mathcal C)/pK_0(calC)/pK_0(mathcal C),calC),
+In K_0(C)/pK_0(calC)/pK_0(C),
 [
   [Y]^p = sum_{i=1}^{p-1}i[F_i(Y)].
 ]
@@ -1099,7 +1099,7 @@ An exact strong monoidal sigma-semilinear functor still preserves
 Frobenius--Perron dimension: it sends nonzero objects to nonzero
 objects (from mathbf 1↪bf1↪ X ⊗  X^*), so
 composing with FP dimension gives a positive normalised character on
-K_0(mathcal C);calC); the FP characterization forces it to be the FP
+K_0(C); the FP characterization forces it to be the FP
 dimension of the source.  In particular
 [
  d(Phi(X)) = d(X).
@@ -1107,10 +1107,10 @@ dimension of the source.  In particular
 
 [first-component inequality]
 
-Let Sinmathcal CcalC be simple and Aboxtimes B a composition
+Let SinC be simple and Aboxtimes B a composition
 factor of Phi(S).  Then d(A)le d(S).  If equality holds then
-Phi(S)simeq Aboxtimes B, B is invertible, and
-Sinmathcal C_calC_{ex} (the subcategory on which the
+Phi(S)~= Aboxtimes B, B is invertible, and
+SinC_{ex} (the subcategory on which the
 ordinary Frobenius functor is exact).
 
 
@@ -1122,13 +1122,13 @@ Equality. If d(A)=d(S) then the FP decomposition sum is a
 single term with d(B)=1, so B is invertible and Phi(S) is
 simple of the form Aboxtimes B.
 
-Sinmathcal C_calC_{ex.}  Let Q_A be the
+SinC_{ex.}  Let Q_A be the
 projective cover of A.  Over k algebraically closed,
 dim_kHom(Q_A,X) = [X:A].  Applying (eq:phi-evaluation) to
 S and X=S^{ ⊗  q}:
 [
- Θ(Hom_{mathcal C}calC(Q_A,S^{ ⊗  q}))
- cong B.
+ Θ(Hom_{C},S^{ ⊗  q}))
+ ~= B.
 ]
 Θ preserves categorical dimension, so its argument has
 categorical dimension equal to that of B, which is nonzero (its
@@ -1143,23 +1143,23 @@ using d(F(Y_{t-1}))ge d(Y_t) and d(ell_{i_t})ge1:
  d(Y_{t-1})ge d(F(Y_{t-1}))ge d(Y_t).
 ]
 But d(Y_r)ge d(A)=d(S)=d(Y_0), so all inequalities are equalities;
-in particular d(F(S))=d(S), so Sinmathcal C_calC_{ex}.
+in particular d(F(S))=d(S), so SinC_{ex}.
 
 
 ## The finite graph
 
 Let N be the number of simple isomorphism classes in
-mathcal C.calC.  Form a directed graph on those classes by arrow
+C.  Form a directed graph on those classes by arrow
 Sto A whenever Aboxtimes B appears in some composition factor
 of Phi(S).
 
 Every vertex has at least one outgoing arrow.  By
 cref{lem:first-component-inequality}, dimension is nonincreasing
 along arrows.  On a directed cycle, dimension is constant, all
-vertices belong to mathcal C_calC_{ex}, and each vertex has
+vertices belong to C_{ex}, and each vertex has
 exactly one outgoing arrow.  Hence a path entering a cycle is
 trapped inside it.  A path of length N visits N+1 vertices and
-so hits a cycle.  Its endpoint is in mathcal C_calC_{ex}.
+so hits a cycle.  Its endpoint is in C_{ex}.
 A schematic path is drawn in cref{fig:dimension-descent}.
 
 [!htbp]
@@ -1192,55 +1192,55 @@ centering
   draw[edge] (B) -- (C);
   draw[edge] (C) -- (A);
   node[align=center] at (-2.8,-0.95)
-    {S→ S' implies d(S')leq d(S)};
+    {S→ S' implies d(S')<= d(S)};
   node[align=center] at (1.83,-2.10)
-    {A,B,Cinmathcal C_calC_{ex}[2pt]
+    {A,B,CinC_{ex}[2pt]
      unique outgoing neighbor at each cycle vertex};
 
 caption{A schematic path in the graph of simple objects, with an
 illustrative three-vertex cycle.  Dimension is nonincreasing along
 every arrow; arrows before the cycle may also preserve dimension.
 On a cycle, cref{lem:first-component-inequality} gives equality,
-membership in mathcal C_calC_{ex}, and a unique outgoing
+membership in C_{ex}, and a unique outgoing
 neighbor at every vertex, so the path cannot leave the cycle.}
 
 
 
 ## Iteration and Serre closure
 
-Let sigma(a)=a^q.  For a k-linear category mathcal A,calA, let
-mathcal A^calA^{[sigma]} have the same objects and additive morphism
+Let sigma(a)=a^q.  For a k-linear category A, let
+A^{[sigma]} have the same objects and additive morphism
 groups but scalar action twisted by sigma^{-1}.  Then
-sigma-semilinear functors out of mathcal AcalA = k-linear
-functors out of mathcal A^calA^{[sigma]}, and
-(mathcal AcalAboxtimesmathcal B)^calB)^{[sigma]}
- = mathcal A^calA^{[sigma]}boxtimesmathcal
+sigma-semilinear functors out of A = k-linear
+functors out of A^{[sigma]}, and
+(A B)^calB)^{[sigma]}
+ = A^{[sigma]}boxtimesmathcal
  B^calB^{[sigma]}, so products of sigma-semilinear functors are
 sigma-semilinear.
 
-Each Ver_{p^s}(k) is defined over mathbb F_p;bbF_p; scalar transport
-along bmapsto b^{p^a} is an exact strong symmetric sigma^a-
+Each Ver_{p^s}(k) is defined over F_p; scalar transport
+along b|-> b^{p^a} is an exact strong symmetric sigma^a-
 semilinear autoequivalence J_{sigma^a} of every
 Ver_{p^s}(k).
 
 Define Psi_0=Id, Psi_1=Phi, and
 
  Psi_{j+1} = (Phiboxtimes J_sigma^{boxtimes j})circPsi_j
- :mathcal CcalCtomathcal CcalCboxtimesmathcal W^calW^{boxtimes(j+1)}.
+ :C CcalCboxtimesW^{boxtimes(j+1)}.
 
 By induction each Psi_j is exact, strong symmetric monoidal,
 and sigma^j-semilinear.
 
 [first components after N iterations]
 
-Let Psi_N :mathcal CcalCtomathcal CcalCboxtimes
-mathcal W^calW^{boxtimes N} be as above.  Then every composition
+Let Psi_N :C CcalCboxtimes
+W^{boxtimes N} be as above.  Then every composition
 factor Aboxtimes B_1boxtimes...boxtimes B_N of
-Psi_N(X) has Ainmathcal C_calC_{ex}.
+Psi_N(X) has AinC_{ex}.
 
 
 Proof. 
-Exactness of Phi plus the path bound on mathcal CcalC (any first
+Exactness of Phi plus the path bound on C (any first
 component of one iteration is a first component of one further
 edge); induction on N, starting with simple objects (where the
 path argument applies) and finishing with composition series.
@@ -1248,84 +1248,84 @@ Autoequivalences on other factors send simples to simples and
 don't touch the first component.
 
 
-Let mathcal D⊆calD⊆mathcal CcalC be the full subcategory whose
-simple composition factors lie in mathcal C_calC_{ex}.  This
-is the Serre closure of mathcal C_calC_{ex}.
+Let D⊆calD⊆C be the full subcategory whose
+simple composition factors lie in C_{ex}.  This
+is the Serre closure of C_{ex}.
 
 [Serre closure inherits tensor structure]
 
-mathcal DcalD is closed under tensor products, duals, extensions, and
+D is closed under tensor products, duals, extensions, and
 contains the unit; it is finite and has enough projectives; it
 carries a rigid symmetric tensor structure inherited from
-mathcal C.calC.  Moreover the functor Psi_N factors through
+C.  Moreover the functor Psi_N factors through
 [
- Psi_N :mathcal CcalCto mathcal DcalDboxtimes
- mathcal W^calW^{boxtimes N}.
+ Psi_N :C D
+ W^{boxtimes N}.
 ]
 
 
 Proof. 
 Closed under tensor products: biexactness gives tensor-product
-filtrations, and mathcal C_calC_{ex} is a tensor
+filtrations, and C_{ex} is a tensor
 subcategory closed under subquotients (Etingof--Ostrik 2021,
-Prop 7.4).  Duality preserves mathcal DcalD by exactness.
+Prop 7.4).  Duality preserves D by exactness.
 
 Finiteness, projectives: concretely, write
-mathcal CcalCsimeq H-mod with H basic finite-dimensional;
+C~= H-mod with H basic finite-dimensional;
 let e be the idempotent summing primitive idempotents of the
-non-mathcal C_calC_{ex} simples; then
-mathcal DcalDsimeq (H/HeH)-mod by removing the
+non-C_{ex} simples; then
+D~= (H/HeH)-mod by removing the
 e-isotypic parts, and H/HeH is finite-dimensional and finite
-projective dimension, so mathcal DcalD is finite with enough
+projective dimension, so D is finite with enough
 projectives.
 
-Factoring through mathcal D:calD: cref{lem:first-components}.
+Factoring through D:calD: cref{lem:first-components}.
 
 
 % =================================================================
-# Finishing the proof: a fiber functor on mathcal DcalD
+# Finishing the proof: a fiber functor on D
 
 % =================================================================
 
-## The fiber functor on mathcal DcalD
+## The fiber functor on D
 
 We need an exact strong symmetric monoidal E:mathcal
 DcalDtoVer_{p^n}(k) for some fixed n.
 
 Case p>2.: 
-mathcal C_calC_{ex} is Frobenius-exact, so by
+C_{ex} is Frobenius-exact, so by
 Etingof--Ostrik (2021, Theorem 8.1) it has a fiber functor
-mathcal C_calC_{ex}toVer_p(k).  If p>2, the Serre closure
-of mathcal C_calC_{ex} equals mathcal C_calC_{ex}
-(Etingof--Ostrik 2021, Corollary 9.5).  So mathcal D=calD=mathcal
-C_calC_{ex} and we already have E:mathcal DcalDtoVer_p(k).
+C_{ex}toVer_p(k).  If p>2, the Serre closure
+of C_{ex} equals C_{ex}
+(Etingof--Ostrik 2021, Corollary 9.5).  So D=
+C_calC_{ex} and we already have E:D
 
 Case p=2.: 
-The fiber functor mathcal C_calC_{ex}toVer_2(k)=Vec_k is a
-k-linear fiber functor.  But mathcal C_calC_{ex}⊆
-mathcal DcalD contains every simple of mathcal DcalD by definition,
-and mathcal C_calC_{ex} is Frobenius-exact.  Etingof--Gelaki
+The fiber functor C_{ex}toVer_2(k)=Vec_k is a
+k-linear fiber functor.  But C_{ex}⊆
+D contains every simple of D by definition,
+and C_{ex} is Frobenius-exact.  Etingof--Gelaki
 (2021, Theorem 2.21(2)) then extends it to
-E:mathcal DcalDtoVer_4^+(k)⊆Ver_4(k).
+E:D+(k)⊆Ver_4(k).
 (This is also Etingof--Ostrik 2021, Corollary 9.8.)
 
 So in all cases:
 [
- E:mathcal DcalD → Ver_{p^n}(k), 
+ E:D → Ver_{p^n}(k), 
  n = 1 & p>2, 2 & p=2.
 ]
 
 ## Combining factors
 
-Set n=max(2,r) and mathcal ZcalZ = Ver_{p^n}(k).  The tower
+Set n=max(2,r) and Z = Ver_{p^n}(k).  The tower
 inclusions Ver_{p^r}(k)⊆Ver_{p^n}(k)
 (Benson--Etingof--Ostrik 2023, Theorem 4.34) give a k-linear exact
-strong symmetric monoidal I:mathcal WcalWtomathcal Z.calZ.
+strong symmetric monoidal I:W Z.calZ.
 
-The functors E:mathcal DcalDtomathcal ZcalZ and I:mathcal WcalWto
-mathcal ZcalZ combine, by cref{lem:combine-functors}, into
+The functors E:D ZcalZ and I:W
+Z combine, by cref{lem:combine-functors}, into
 [
- H:mathcal DcalDboxtimesmathcal W^calW^{boxtimes N}tomathcal Z,calZ,
+ H:D W^calW^{boxtimes N}toZ,
  
  H(Dboxtimes W_1boxtimes...boxtimes W_N)
  = E(D) ⊗  I(W_1) ⊗ ... ⊗  I(W_N).
@@ -1334,13 +1334,13 @@ H is exact and strong symmetric monoidal.
 
 ## Killing the scalar twist
 
-The composite HPsi_N :mathcal CcalCtomathcal ZcalZ is
+The composite HPsi_N :C ZcalZ is
 sigma^N-semilinear (each iteration multiplies semilinearity by
-sigma).  Let J_{sigma^{-N}} be scalar transport on mathcal ZcalZ
-along bmapsto b^{p^{-N}}.  Then
+sigma).  Let J_{sigma^{-N}} be scalar transport on Z
+along b|-> b^{p^{-N}}.  Then
 [
- mathcal FcalF := J_{sigma^{-N}}circ HcircPsi_N :
- mathcal C→calC→mathcal ZcalZ
+ F := J_{sigma^{-N}}circ HcircPsi_N :
+ C→calC→Z
 ]
 is k-linear, exact, strong symmetric monoidal.
 
@@ -1348,7 +1348,7 @@ is k-linear, exact, strong symmetric monoidal.
 
 [exact strong monoidal with simple unit is faithful]
 
-Let F:mathcal CcalCtomathcal DcalD be an exact strong symmetric
+Let F:C DcalD be an exact strong symmetric
 monoidal functor between finite symmetric tensor categories.  Then
 F is faithful.
 
@@ -1358,12 +1358,12 @@ Suppose Xne0.  The coevaluation
 mathbf 1bf1to X ⊗  X^* is nonzero (triangle identity) and by
 simplicity of mathbf 1bf1 it is injective; applying exact F shows
 F(X)ne0.  For a nonzero f:Xto Y: exactness gives
-imF(f)cong F(imf), and
+imF(f)~= F(imf), and
 imfne0, so F(f)ne0.
 
 
-Applying cref{lem:faithful} to mathcal FcalF shows mathcal FcalF is
-faithful.  Hence mathcal F:calF:mathcal CcalCtoVer_{p^n}(k) is the
+Applying cref{lem:faithful} to F shows F is
+faithful.  Hence F:calF:C{p^n}(k) is the
 required fiber functor, and cref{thm:main} follows.
 
 % =================================================================
@@ -1376,14 +1376,14 @@ motivation for proving cref{thm:main}.
 
 ## Incompressible categories
 
-Recall that mathcal CcalC is incompressible if every
-k-linear exact strong symmetric monoidal functor from mathcal CcalC
+Recall that C is incompressible if every
+k-linear exact strong symmetric monoidal functor from C
 to a symmetric tensor category over k is fully faithful.
 
 [classification of finite incompressible]
 
 Let k be algebraically closed of characteristic p>0.  A finite
-symmetric tensor category mathcal CcalC over k is incompressible if
+symmetric tensor category C over k is incompressible if
 and only if it is k-linearly equivalent as a symmetric tensor
 category to one of the following, according to p:
 [
@@ -1407,16 +1407,16 @@ For the Verlinde full and plus categories, see Benson--Etingof--
 Ostrik (2023), Theorems 4.71 and 4.72(iii).
 
 Direction ⇒: take a fiber functor
-F:mathcal CcalCtoVer_{p^n}(k) from cref{thm:main}, let
-mathcal IcalI be the image's full subcategory of subquotients.
+F:C{p^n}(k) from cref{thm:main}, let
+I be the image's full subcategory of subquotients.
 Then F corestricts to a surjective-in-the-tensor-category-sense
-functor onto mathcal IcalI (Etingof--Gelaki--Nikshych--Ostrik 2015,
+functor onto I (Etingof--Gelaki--Nikshych--Ostrik 2015,
 Definition 1.8.18, Prop 1.8.19, Section 6.3).  Incompressibility
-of mathcal CcalC forces this corestriction to be fully faithful.
+of C forces this corestriction to be fully faithful.
 The two FP-dimension inequalities of finiteness (inclusion vs
 surjection) then force equality, hence an equivalence.
 Benson--Etingof--Ostrik 2023, Corollary 4.61 then restricts
-mathcal IcalI to a full or plus sub-Verlinde at height le n.
+I to a full or plus sub-Verlinde at height le n.
 Collecting cases gives the stated list.
 
 
@@ -1432,12 +1432,12 @@ finite case of Conjecture~B of
 [uniqueness in characteristic two]
 
 Let k be algebraically closed of characteristic two and
-mathcal CcalC a finite symmetric tensor category.  Then
-mathcal CcalCtoVer_{2^∞}(k) :=∪_nVer_{2^n}(k) has
+C a finite symmetric tensor category.  Then
+C{2^∞}(k) :=∪_nVer_{2^n}(k) has
 exactly one fiber functor up to monoidal natural isomorphism; its
 class contains a representative into a finite stage
 Ver_{2^n}(k); and for each fixed n there is at most one fiber
-functor mathcal CcalCtoVer_{2^n}(k) up to monoidal natural
+functor C{2^n}(k) up to monoidal natural
 isomorphism.
 
 
@@ -1453,33 +1453,33 @@ inclusion; naturality and tensor compatibility hold by faithfulness.
 
 ## Tannaka reconstruction over a Verlinde level
 
-Let mathcal VcalV be a finite symmetric tensor category.  The
-fundamental group pi(mathcal V)calV) :=
-Aut^{ ⊗ }(Id_mathcal V)calV) acts
-canonically on Ind(mathcal V).calV).  A
-mathcal V-groupcalV-group is an internal affine group scheme G with
-a homomorphism phi:pi(mathcal V)calV)to G whose induced coaction
+Let V be a finite symmetric tensor category.  The
+fundamental group pi(V) :=
+Aut^{ ⊗ }(Id_V) acts
+canonically on Ind(V).  A
+V-groupcalV-group is an internal affine group scheme G with
+a homomorphism phi:pi(V) G whose induced coaction
 matches the canonical one.
 
 [reconstruction over a Verlinde level]
 
 Let k be algebraically closed of characteristic p>0, mathcal
-CcalC finite symmetric tensor, and F:mathcal CcalCto
-mathcal V=calV=Ver_{p^n}(k) a fiber functor (from cref{thm:main}).
-Then there is a mathcal V-groupcalV-group (G,phi) with
-mathcal CcalCsimeqRep(G,phi) over mathcal V,calV, equivalent to
+CcalC finite symmetric tensor, and F:C
+V={p^n}(k) a fiber functor (from cref{thm:main}).
+Then there is a V-groupcalV-group (G,phi) with
+C~=Rep(G,phi) over V, equivalent to
 F under the forgetful functor.  One may take
 G=Aut^{ ⊗ }(F) and
-phi:pi(mathcal V)calV)toAut^{ ⊗ }(F) the
+phi:pi(V){ ⊗ }(F) the
 canonical homomorphism.
 
 
 Proof. 
-Cref{lem:modules-finite-alg} makes mathcal C,calC, together with
-mathcal V=calV=Ver_{p^n}(k), a ``pretannakian category'' in the
+Cref{lem:modules-finite-alg} makes C, together with
+V={p^n}(k), a ``pretannakian category'' in the
 sense of Coulembier--Etingof--Ostrik (2024).  The chosen F is a
 tensor functor, and their Theorem 4.2.1 produces the stated
-mathcal V-group;calV-group; conversely, forgetting G-structure gives the
+V-group;calV-group; conversely, forgetting G-structure gives the
 inverse functor.  Composition is the equivalence.
 
 
@@ -1489,7 +1489,7 @@ All classification and existence assertions above are confined to
 finite categories.  Uniqueness is asserted only in characteristic
 two, both in the tower union and at each fixed finite stage where a
 fiber functor exists.  Cref{thm:main} supplies some finite height
-n depending on mathcal C;calC; it makes no claim of existence
+n depending on C; it makes no claim of existence
 at a prescribed height.  In the reconstruction, G is affine but
 neither its finiteness nor its finite-type property is used or
 claimed.