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The Petrie symmetrie functions and Murnaghan–Nakayama rules

Darij Grinberg

4 February 2020

Institut Mittag–Leffler, Djursholm, Sweden

slides: http://www.cip.ifi.lmu.de/~grinberg/algebra/

djursholm2020.pdf paper: http:

//www.cip.ifi.lmu.de/~grinberg/algebra/petriesym.pdf overview: http:

//www.cip.ifi.lmu.de/~grinberg/algebra/fps20pet.pdf

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Manifest

What you are going to see:

A new family (G(k,m))m≥0 of symmetric functions for eachk >0. (So, a family of families.)

It “interpolates” between thee’s and the h’s in a sense.

Various nice properties if I do say so myself.

A proof (sketch) of a conjecture coming from algebraic groups.

A source of homework exercises for your symmetric functions class.

What you arenot going to see:

Meaning.

Theories.

(mostly) actual combinatorics (algorithms, bijections, etc.).

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Manifest

What you are going to see:

A new family (G(k,m))m≥0 of symmetric functions for eachk >0. (So, a family of families.)

It “interpolates” between thee’s and the h’s in a sense.

Various nice properties if I do say so myself.

A proof (sketch) of a conjecture coming from algebraic groups.

A source of homework exercises for your symmetric functions class.

What you arenot going to see:

Meaning.

Theories.

(mostly) actual combinatorics (algorithms, bijections, etc.).

2 / 43

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Symmetric functions: notation, 1

We will use standard notations for symmetric functions, such as used in:

Richard Stanley, Enumerative Combinatorics, volume 2, CUP 2001.

D.G. and Victor Reiner,Hopf algebras in Combinatorics, 2012-2020+.

Let k be a commutative ring (ZandQ will suffice).

Let N:={0,1,2, . . .}.

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Symmetric functions: notation, 1

We will use standard notations for symmetric functions, such as used in:

Richard Stanley, Enumerative Combinatorics, volume 2, CUP 2001.

D.G. and Victor Reiner,Hopf algebras in Combinatorics, 2012-2020+.

Let k be a commutative ring (ZandQ will suffice).

Let N:={0,1,2, . . .}.

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Symmetric functions: notation, 2

A weak composition means a sequence (α1, α2, α3, . . .)∈N such that all i 0 satisfy αi = 0.

We let WCbe the set of all weak compositions.

We writeαi for the i-th entry of a weak compositionα.

The sizeof a weak compositionα is defined to be

|α|:=α123+· · ·.

A partitionmeans a weak compositionα satisfying α1≥α2 ≥α3 ≥ · · ·.

A partition of n means a partitionα with |α|=n.

We let Par denote the set of all partitions. For eachn ∈Z, we let Parn denote the set of all partitions of n.

We often omit trailing zeroes from partitions: e.g., (3,2,1,0,0,0, . . .) = (3,2,1) = (3,2,1,0).

The partition (0,0,0, . . .) = () is called theempty partition and denoted by ∅.

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Symmetric functions: notation, 2

A weak composition means a sequence (α1, α2, α3, . . .)∈N such that all i 0 satisfy αi = 0.

We let WCbe the set of all weak compositions.

We writeαi for the i-th entry of a weak compositionα.

The sizeof a weak compositionα is defined to be

|α|:=α123+· · ·.

A partitionmeans a weak compositionα satisfying α1≥α2 ≥α3 ≥ · · ·.

A partition of n means a partitionα with |α|=n.

We letPardenote the set of all partitions. For eachn ∈Z, we let Parn denote the set of all partitions of n.

We often omit trailing zeroes from partitions: e.g., (3,2,1,0,0,0, . . .) = (3,2,1) = (3,2,1,0).

The partition (0,0,0, . . .) = () is called theempty partition and denoted by ∅.

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Symmetric functions: notation, 2

A weak composition means a sequence (α1, α2, α3, . . .)∈N such that all i 0 satisfy αi = 0.

We let WCbe the set of all weak compositions.

We writeαi for the i-th entry of a weak compositionα.

The sizeof a weak compositionα is defined to be

|α|:=α123+· · ·.

A partitionmeans a weak compositionα satisfying α1≥α2 ≥α3 ≥ · · ·.

A partition of n means a partitionα with |α|=n.

We letPardenote the set of all partitions. For eachn ∈Z, we let Parn denote the set of all partitions of n.

We often omit trailing zeroes from partitions: e.g., (3,2,1,0,0,0, . . .) = (3,2,1) = (3,2,1,0).

The partition (0,0,0, . . .) = () is called theempty partition and denoted by ∅.

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Symmetric functions: notation, 3

We will use the notationmk for “m,m, . . . ,m

| {z }

ktimes

” in partitions.

(For example, 2,14

= (2,1,1,1,1).)

For any weak composition α, we let xα denote the monomial x1α1x2α2x3α3· · ·. It has degree|α|.

The ring k [[x1,x2,x3, . . .]] consists of formal infinite k-linear combinations of monomials xα. These combinations are called formal power series.

The symmetric functionsare the formal power series f ∈k [[x1,x2,x3, . . .]] that are

of bounded degree (i.e., all monomials in f have degrees

<N for someN=Nf);

symmetric(i.e., permuting the xi does not changef). We let

Λ={symmetric functions f ∈k [[x1,x2,x3, . . .]]}. This is a k-subalgebra of k [[x1,x2,x3, . . .]], graded by the degree.

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Symmetric functions: notation, 3

We will use the notationmk for “m,m, . . . ,m

| {z }

ktimes

” in partitions.

(For example, 2,14

= (2,1,1,1,1).)

For any weak composition α, we letxα denote the monomial x1α1x2α2x3α3· · ·. It has degree|α|.

The ring k [[x1,x2,x3, . . .]] consists of formal infinite k-linear combinations of monomials xα. These combinations are called formal power series.

The symmetric functionsare the formal power series f ∈k [[x1,x2,x3, . . .]] that are

of bounded degree (i.e., all monomials in f have degrees

<N for someN=Nf);

symmetric(i.e., permuting the xi does not changef).

We let

Λ={symmetric functions f ∈k [[x1,x2,x3, . . .]]}. This is a k-subalgebra of k [[x1,x2,x3, . . .]], graded by the degree.

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Symmetric functions: notation, 3

We will use the notationmk for “m,m, . . . ,m

| {z }

ktimes

” in partitions.

(For example, 2,14

= (2,1,1,1,1).)

For any weak composition α, we letxα denote the monomial x1α1x2α2x3α3· · ·. It has degree|α|.

The ring k [[x1,x2,x3, . . .]] consists of formal infinite k-linear combinations of monomials xα. These combinations are called formal power series.

The symmetric functionsare the formal power series f ∈k [[x1,x2,x3, . . .]] that are

of bounded degree (i.e., all monomials in f have degrees

<N for someN=Nf);

symmetric(i.e., permuting the xi does not changef).

We let

Λ ={symmetric functions f ∈k [[x1,x2,x3, . . .]]}. This is a k-subalgebra of k [[x1,x2,x3, . . .]], graded by the degree.

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Symmetric functions: notation, 3

We will use the notationmk for “m,m, . . . ,m

| {z }

ktimes

” in partitions.

(For example, 2,14

= (2,1,1,1,1).)

For any weak composition α, we letxα denote the monomial x1α1x2α2x3α3· · ·. It has degree|α|.

The ring k [[x1,x2,x3, . . .]] consists of formal infinite k-linear combinations of monomials xα. These combinations are called formal power series.

The symmetric functionsare the formal power series f ∈k [[x1,x2,x3, . . .]] that are

of bounded degree (i.e., all monomials in f have degrees

<N for someN=Nf);

symmetric(i.e., permuting the xi does not changef).

We let

Λ={symmetric functions f ∈k [[x1,x2,x3, . . .]]}. This is a k-subalgebra of k [[x1,x2,x3, . . .]], graded by the degree.

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Symmetric functions: m

The k-module Λ has several bases indexed by the set Par.

The monomial basis(mλ)λ∈Par:

For each partitionλ, we define themonomial symmetric function mλ ∈Λ by

mλ = X

αis a weak composition;

αcan be obtained fromλ by permuting entries

xα.

For example: m(2,2,1)= X

i<j<k

xi2xj2xk+ X

i<j<k

xi2xjxk2+ X

i<j<k

xixj2xk2.

The family (mλ)λ∈Par is a basis of the k-module Λ, called the monomial basis.

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Symmetric functions: m

The k-module Λ has several bases indexed by the set Par.

The monomial basis(mλ)λ∈Par:

For each partitionλ, we define themonomial symmetric functionmλ ∈Λ by

mλ = X

αis a weak composition;

αcan be obtained fromλ by permuting entries

xα.

For example:

m(2,2,1)= X

i<j<k

xi2xj2xk+ X

i<j<k

xi2xjxk2+ X

i<j<k

xixj2xk2.

The family (mλ)λ∈Par is a basis of the k-module Λ, called the monomial basis.

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Symmetric functions: m

The k-module Λ has several bases indexed by the set Par.

The monomial basis(mλ)λ∈Par:

For each partitionλ, we define themonomial symmetric functionmλ ∈Λ by

mλ = X

αis a weak composition;

αcan be obtained fromλ by permuting entries

xα.

For example:

m(2,2,1)= X

i<j<k

xi2xj2xk+ X

i<j<k

xi2xjxk2+ X

i<j<k

xixj2xk2.

The family (mλ)λ∈Par is a basis of the k-module Λ, called the monomial basis.

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Symmetric functions: m

The k-module Λ has several bases indexed by the set Par.

The monomial basis(mλ)λ∈Par:

For each partitionλ, we define themonomial symmetric functionmλ ∈Λ by

mλ = X

αis a weak composition;

αcan be obtained fromλ by permuting entries

xα.

For example:

m(2,2,1)= X

i<j<k

xi2xj2xk+ X

i<j<k

xi2xjxk2+ X

i<j<k

xixj2xk2.

The family (mλ)λ∈Par is a basis of the k-module Λ, called the monomial basis.

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Symmetric functions: h

The complete basis (hλ)λ∈Par:

For eachn∈Z, define the complete homogeneous symmetric function hn by

hn = X

i1≤i2≤···≤in

xi1xi2· · ·xin = X

α∈WC;

|α|=n

xα = X

λ∈Parn

mλ.

For example,

h1 =x1+x2+x3+· · · ; h2 =X

i≤j

xixj =X

i

xi2+X

i<j

xixj; h0 = 1;

hn= 0 for all n<0.

For each partitionλ, we define

hλ =hλ1hλ2hλ3· · · ∈Λ. The family (hλ)λ∈Par is a basis of the k-module Λ.

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Symmetric functions: h

The complete basis (hλ)λ∈Par:

For eachn∈Z, define the complete homogeneous symmetric function hn by

hn = X

i1≤i2≤···≤in

xi1xi2· · ·xin = X

α∈WC;

|α|=n

xα = X

λ∈Parn

mλ.

For example,

h1 =x1+x2+x3+· · · ; h2 =X

i≤j

xixj =X

i

xi2+X

i<j

xixj; h0 = 1;

hn= 0 for all n<0.

For each partitionλ, we define

hλ =hλ1hλ2hλ3· · · ∈Λ.

The family (hλ)λ∈Par is a basis of the k-module Λ.

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Symmetric functions: h

The complete basis (hλ)λ∈Par:

For eachn∈Z, define the complete homogeneous symmetric function hn by

hn = X

i1≤i2≤···≤in

xi1xi2· · ·xin = X

α∈WC;

|α|=n

xα = X

λ∈Parn

mλ.

For example,

h1 =x1+x2+x3+· · · ; h2 =X

i≤j

xixj =X

i

xi2+X

i<j

xixj; h0 = 1;

hn= 0 for all n<0.

For each partitionλ, we define

hλ =hλ1hλ2hλ3· · · ∈Λ.

The family (hλ)λ∈Par is a basis of the k-module Λ.

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Symmetric functions: e

The elementary basis(eλ)λ∈Par:

For eachn∈Z, define the elementary symmetric function en

by

en= X

i1<i2<···<in

xi1xi2· · ·xin = X

α∈WC∩{0,1};

|α|=n

xα=m(1n).

For example,

e1 =x1+x2+x3+· · · ; e2 =X

i<j

xixj; e0 = 1;

en= 0 for all n<0.

For each partitionλ, we define

eλ=eλ1eλ2eλ3· · · ∈Λ.

The family (eλ)λ∈Par is a basis of the k-module Λ.

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Symmetric functions: e

The elementary basis(eλ)λ∈Par:

For eachn∈Z, define the elementary symmetric function en

by

en= X

i1<i2<···<in

xi1xi2· · ·xin = X

α∈WC∩{0,1};

|α|=n

xα=m(1n).

For example,

e1 =x1+x2+x3+· · · ; e2 =X

i<j

xixj; e0 = 1;

en= 0 for all n<0.

For each partitionλ, we define

eλ=eλ1eλ2eλ3· · · ∈Λ.

The family (eλ)λ∈Par is a basis of the k-module Λ.

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Symmetric functions: e

The elementary basis(eλ)λ∈Par:

For eachn∈Z, define the elementary symmetric function en

by

en= X

i1<i2<···<in

xi1xi2· · ·xin = X

α∈WC∩{0,1};

|α|=n

xα=m(1n).

For example,

e1 =x1+x2+x3+· · · ; e2 =X

i<j

xixj; e0 = 1;

en= 0 for all n<0.

For each partitionλ, we define

eλ=eλ1eλ2eλ3· · · ∈Λ.

The family (eλ)λ∈Par is a basis of the k-module Λ.

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Symmetric functions: p

The power-sum symmetric functionspn:

For each positive integer n, define the power-sum symmetric function pn by

pn=x1n+x2n+x3n+· · ·=m(n).

We can make a basis out of (products of) pn’s when k is a Q-algebra.

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Symmetric functions: p

The power-sum symmetric functionspn:

For each positive integer n, define the power-sum symmetric function pn by

pn=x1n+x2n+x3n+· · ·=m(n).

We can make a basis out of (products of) pn’s when k is a Q-algebra.

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Symmetric functions: s

The Schur basis(sλ)λ∈Par:

For each partitionλ, we can define theSchur function sλ in many equivalent ways, e.g.:

We have

sλ = X

T is a semistandard Young tableau of shapeλ

xT,

where xT denotes the monomial obtained by multiplying thexi for all entriesi of T.

Ifλ= (λ1, λ2, . . . , λ`), then sλ= det

(hλi−i+j)1≤i≤`,1≤j≤`

(thefirst Jacobi–Trudi formula).

The family (sλ)λ∈Par is a basis of the k-module Λ.

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Symmetric functions: s

The Schur basis(sλ)λ∈Par:

For each partitionλ, we can define theSchur function sλ in many equivalent ways, e.g.:

We have

sλ = X

T is a semistandard Young tableau of shapeλ

xT,

where xT denotes the monomial obtained by multiplying thexi for all entriesi of T.

Ifλ= (λ1, λ2, . . . , λ`), then sλ= det

(hλi−i+j)1≤i≤`,1≤j≤`

(thefirst Jacobi–Trudi formula).

The family (sλ)λ∈Par is a basis of the k-module Λ.

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Petrie functions: definition of G(k) For any positive integer k, set

G(k)

= X

α∈WC;

αi<kfor alli

xα

=X

(all monomials whose exponents are all <k)

∈k [[x1,x2,x3, . . .]] (not ∈Λ in general).

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Petrie functions: definition of G(k,m)

For any positive integer k and any m∈N, we let G(k,m)

= X

α∈WC;

|α|=m;

αi<kfor alli

xα

=X

(all degree-m monomials whose exponents are all <k)

∈Λ.

For example, G(3,4) = X

i<j<k<`

xixjxkx`+ X

i<j<k

xi2xjxk + X

i<j<k

xixj2xk

+ X

i<j<k

xixjxk2+X

i<j

xi2xj2

=m(1,1,1,1)+m(2,1,1)+m(2,2).

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Petrie functions: definition of G(k,m)

For any positive integer k and any m∈N, we let G(k,m)

= X

α∈WC;

|α|=m;

αi<kfor alli

xα

=X

(all degree-m monomials whose exponents are all <k)

∈Λ.

For example, G(3,4) = X

i<j<k<`

xixjxkx`+ X

i<j<k

xi2xjxk + X

i<j<k

xixj2xk

+ X

i<j<k

xixjxk2+X

i<j

xi2xj2

=m(1,1,1,1)+m(2,1,1)+m(2,2).

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Petrie functions: basic properties

I named G(k) andG(k,m) the Petrie functions, for reasons that will become clear eventually.

Basic properties(for arbitraryk >0 andm∈N):

G(k) = X

λ∈Par;

λi<kfor alli

mλ =

Y

i=1

xi0+xi1+· · ·+xik−1

.

G(k,m) is them-th degree component ofG(k). G(k,m) = X

λ∈Par;

|λ|=m; λi<kfor alli

mλ.

G(2,m) =em.

G(k,m) =hm whenever k>m. G(m,m) =hm−pm.

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Petrie functions: basic properties

I named G(k) andG(k,m) the Petrie functions, for reasons that will become clear eventually.

Basic properties(for arbitraryk >0 andm∈N):

G(k) = X

λ∈Par;

λi<kfor alli

mλ =

Y

i=1

xi0+xi1+· · ·+xik−1

.

G(k,m) is them-th degree component ofG(k).

G(k,m) = X

λ∈Par;

|λ|=m; λi<kfor alli

mλ.

G(2,m) =em.

G(k,m) =hm whenever k>m. G(m,m) =hm−pm.

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Petrie functions: basic properties

I named G(k) andG(k,m) the Petrie functions, for reasons that will become clear eventually.

Basic properties(for arbitraryk >0 andm∈N):

G(k) = X

λ∈Par;

λi<kfor alli

mλ =

Y

i=1

xi0+xi1+· · ·+xik−1

.

G(k,m) is them-th degree component ofG(k).

G(k,m) = X

λ∈Par;

|λ|=m;

λi<kfor alli

mλ.

G(2,m) =em.

G(k,m) =hm whenever k>m. G(m,m) =hm−pm.

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Petrie functions: basic properties

I named G(k) andG(k,m) the Petrie functions, for reasons that will become clear eventually.

Basic properties(for arbitraryk >0 andm∈N):

G(k) = X

λ∈Par;

λi<kfor alli

mλ =

Y

i=1

xi0+xi1+· · ·+xik−1

.

G(k,m) is them-th degree component ofG(k).

G(k,m) = X

λ∈Par;

|λ|=m;

λi<kfor alli

mλ.

G(2,m) =em.

G(k,m) =hm whenever k>m. G(m,m) =hm−pm.

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Petrie functions: basic properties

I named G(k) andG(k,m) the Petrie functions, for reasons that will become clear eventually.

Basic properties(for arbitraryk >0 andm∈N):

G(k) = X

λ∈Par;

λi<kfor alli

mλ =

Y

i=1

xi0+xi1+· · ·+xik−1

.

G(k,m) is them-th degree component ofG(k).

G(k,m) = X

λ∈Par;

|λ|=m;

λi<kfor alli

mλ.

G(2,m) =em.

G(k,m) =hm wheneverk >m.

G(m,m) =hm−pm.

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Petrie functions: basic properties

I named G(k) andG(k,m) the Petrie functions, for reasons that will become clear eventually.

Basic properties(for arbitraryk >0 andm∈N):

G(k) = X

λ∈Par;

λi<kfor alli

mλ =

Y

i=1

xi0+xi1+· · ·+xik−1

.

G(k,m) is them-th degree component ofG(k).

G(k,m) = X

λ∈Par;

|λ|=m;

λi<kfor alli

mλ.

G(2,m) =em.

G(k,m) =hm wheneverk >m.

G(m,m) =hm−pm.

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Petrie functions: basic properties

I named G(k) andG(k,m) the Petrie functions, for reasons that will become clear eventually.

Basic properties(for arbitraryk >0 andm∈N):

G(k) = X

λ∈Par;

λi<kfor alli

mλ =

Y

i=1

xi0+xi1+· · ·+xik−1

.

G(k,m) is them-th degree component ofG(k).

G(k,m) = X

λ∈Par;

|λ|=m;

λi<kfor alli

mλ.

G(2,m) =em.

G(k,m) =hm wheneverk >m.

G(m,m) =hm−pm.

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Petrie functions and the coproduct of Λ This is for the friends of Hopf algebras:

∆ (G(k,m)) =

m

X

i=0

G(k,i)⊗G(k,m−i) for eachk >0 andm∈N.

Here, ∆is the comultiplicationof Λ, defined to be the k-algebra homomorphism

∆ : Λ→Λ⊗Λ, en7→

n

X

i=0

ei ⊗en−i.

In terms of alphabets, this says

(G(k,m)) (x1,x2,x3, . . . ,y1,y2,y3, . . .)

=

m

X

i=0

(G(k,i)) (x1,x2,x3, . . .)·(G(k,m−i)) (y1,y2,y3, . . .).

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Petrie functions and the coproduct of Λ This is for the friends of Hopf algebras:

∆ (G(k,m)) =

m

X

i=0

G(k,i)⊗G(k,m−i) for eachk >0 andm∈N.

Here, ∆is the comultiplicationof Λ, defined to be the k-algebra homomorphism

∆ : Λ→Λ⊗Λ, en7→

n

X

i=0

ei ⊗en−i.

In terms of alphabets, this says

(G(k,m)) (x1,x2,x3, . . . ,y1,y2,y3, . . .)

=

m

X

i=0

(G(k,i)) (x1,x2,x3, . . .)·(G(k,m−i)) (y1,y2,y3, . . .).

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Expanding Petries in the Schur basis

We can expand the G(k,m) in the Schur basis (sλ)λ∈Par: e.g., G(4,6) =s(2,1,1,1,1)−s(2,2,1,1)+s(3,3).

Surprisingly, it turns out that all coefficients are in {0,1,−1}.

Better yet: Any product G(k,m)·sµ expands in the Schur basis with coefficients in{0,1,−1}.

Let us see what the coefficients are.

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Expanding Petries in the Schur basis

We can expand the G(k,m) in the Schur basis (sλ)λ∈Par: e.g., G(4,6) =s(2,1,1,1,1)−s(2,2,1,1)+s(3,3).

Surprisingly, it turns out that all coefficients are in {0,1,−1}.

Better yet: Any product G(k,m)·sµ expands in the Schur basis with coefficients in{0,1,−1}.

Let us see what the coefficients are.

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Expanding Petries in the Schur basis

We can expand the G(k,m) in the Schur basis (sλ)λ∈Par: e.g., G(4,6) =s(2,1,1,1,1)−s(2,2,1,1)+s(3,3).

Surprisingly, it turns out that all coefficients are in {0,1,−1}.

Better yet: Any product G(k,m)·sµ expands in the Schur basis with coefficients in{0,1,−1}.

Let us see what the coefficients are.

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Expanding Petries in the Schur basis

We can expand the G(k,m) in the Schur basis (sλ)λ∈Par: e.g., G(4,6) =s(2,1,1,1,1)−s(2,2,1,1)+s(3,3).

Surprisingly, it turns out that all coefficients are in {0,1,−1}.

Better yet: Any product G(k,m)·sµ expands in the Schur basis with coefficients in{0,1,−1}.

Let us see what the coefficients are.

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Petrie numbers

We let [A] denote the truth valueof a statementA (that is, 1 if Ais true, and 0 ifA is false).

Let λ= (λ1, λ2, . . . , λ`)∈Par and

µ= (µ1, µ2, . . . , µ`)∈Par, and letk be a positive integer.

Then, the k-Petrie numberpetk(λ, µ) ofλand µis the integer defined by

petk(λ, µ) = det

([0≤λi −µj −i+j <k])1≤i≤`,1≤j≤`

.

Proposition: We have petk(λ, µ)∈ {0,1,−1} for all λand µ.

Proof idea. Each row of the matrix

([0≤λi −µj −i+j <k])1≤i≤`,1≤j≤` has the form (0,0, . . . ,0

| {z }

azeroes

,1,1, . . . ,1

| {z }

bones

,0,0, . . . ,0

| {z }

czeroes

) for somea,b,c ∈N. Thus, this matrix is the transpose of a Petrie matrix. Hence, its determinant is ∈ {−1,0,1} (byGordon and Wilkinson 1974).

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Petrie numbers

We let [A] denote the truth valueof a statementA (that is, 1 if Ais true, and 0 ifA is false).

Let λ= (λ1, λ2, . . . , λ`)∈Par and

µ= (µ1, µ2, . . . , µ`)∈Par, and letk be a positive integer.

Then, the k-Petrie numberpetk(λ, µ) ofλand µis the integer defined by

petk(λ, µ) = det

([0≤λi −µj −i+j <k])1≤i≤`,1≤j≤`

.

Proposition: We have petk(λ, µ)∈ {0,1,−1} for all λand µ.

Proof idea. Each row of the matrix

([0≤λi −µj −i+j <k])1≤i≤`,1≤j≤` has the form (0,0, . . . ,0

| {z }

azeroes

,1,1, . . . ,1

| {z }

bones

,0,0, . . . ,0

| {z }

czeroes

) for somea,b,c ∈N. Thus, this matrix is the transpose of a Petrie matrix. Hence, its determinant is ∈ {−1,0,1} (byGordon and Wilkinson 1974).

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Petrie numbers

We let [A] denote the truth valueof a statementA (that is, 1 if Ais true, and 0 ifA is false).

Let λ= (λ1, λ2, . . . , λ`)∈Par and

µ= (µ1, µ2, . . . , µ`)∈Par, and letk be a positive integer.

Then, the k-Petrie numberpetk(λ, µ) ofλand µis the integer defined by

petk(λ, µ) = det

([0≤λi −µj −i+j <k])1≤i≤`,1≤j≤`

. For example, for `= 3, we have

petk(λ, µ)

= det

[0λ1µ1<k] [0λ1µ2+ 1<k] [0λ1µ3+ 2<k]

[0λ2µ11<k] [0λ2µ2<k] [0λ2µ3+ 1<k]

[0λ3µ12<k] [0λ3µ21<k] [0λ3µ3<k]

.

For example,

pet4((3,1,1),(2,1)) = det

1 1 0 0 1 1 0 0 1

= 1.

Proposition: We have petk(λ, µ)∈ {0,1,−1} for all λand µ.

Proof idea. Each row of the matrix

([0≤λi −µj −i+j <k])1≤i≤`,1≤j≤` has the form (0,0, . . . ,0

| {z }

azeroes

,1,1, . . . ,1

| {z }

bones

,0,0, . . . ,0

| {z }

czeroes

) for somea,b,c ∈N. Thus, this matrix is the transpose of a Petrie matrix. Hence, its determinant is ∈ {−1,0,1} (byGordon and Wilkinson 1974).

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Petrie numbers

We let [A] denote the truth valueof a statementA (that is, 1 if Ais true, and 0 ifA is false).

Let λ= (λ1, λ2, . . . , λ`)∈Par and

µ= (µ1, µ2, . . . , µ`)∈Par, and letk be a positive integer.

Then, the k-Petrie numberpetk(λ, µ) ofλand µis the integer defined by

petk(λ, µ) = det

([0≤λi −µj −i+j <k])1≤i≤`,1≤j≤`

. Proposition: We have petk(λ, µ)∈ {0,1,−1} for all λand µ.

Proof idea. Each row of the matrix

([0≤λi−µj −i+j <k])1≤i≤`,1≤j≤` has the form (0,0, . . . ,0

| {z }

azeroes

,1,1, . . . ,1

| {z }

bones

,0,0, . . . ,0

| {z }

czeroes

) for somea,b,c ∈N.

Thus, this matrix is the transpose of a Petrie matrix. Hence, its determinant is ∈ {−1,0,1} (by Gordon and Wilkinson 1974).

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Petrie numbers

We let [A] denote the truth valueof a statementA (that is, 1 if Ais true, and 0 ifA is false).

Let λ= (λ1, λ2, . . . , λ`)∈Par and

µ= (µ1, µ2, . . . , µ`)∈Par, and letk be a positive integer.

Then, the k-Petrie numberpetk(λ, µ) ofλand µis the integer defined by

petk(λ, µ) = det

([0≤λi −µj −i+j <k])1≤i≤`,1≤j≤`

. Proposition: We have petk(λ, µ)∈ {0,1,−1} for all λand µ.

Proof idea. Each row of the matrix

([0≤λi−µj −i+j <k])1≤i≤`,1≤j≤` has the form (0,0, . . . ,0

| {z }

azeroes

,1,1, . . . ,1

| {z }

bones

,0,0, . . . ,0

| {z }

czeroes

) for somea,b,c ∈N.

Thus, this matrix is the transpose of a Petrie matrix. Hence, its determinant is ∈ {−1,0,1} (byGordon and Wilkinson 1974).

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Expanding Petries in the Schur basis: the formula

Theorem: Let k be a positive integer. Letµ∈Par. Then, G(k)·sµ= X

λ∈Par

petk(λ, µ)sλ. Thus, for each m∈N, we have

G(k,m)·sµ= X

λ∈Parm+|µ|

petk(λ, µ)sλ.

One proof of the Theorem uses alternants; the other uses the

“semi-skew Cauchy identity” X

λ∈Par

sλ(x)sλ/µ(y) =sµ(x)·

Y

i,j=1

(1−xiyj)−1

=sµ(x)· X

λ∈Par

hλ(x)mλ(y) (for any µ∈Par and for two sets of indeterminates x = (x1,x2,x3, . . .) and y = (y1,y2,y3, . . .)).

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Expanding Petries in the Schur basis: the formula

Theorem: Let k be a positive integer. Letµ∈Par. Then, G(k)·sµ= X

λ∈Par

petk(λ, µ)sλ. Thus, for each m∈N, we have

G(k,m)·sµ= X

λ∈Parm+|µ|

petk(λ, µ)sλ.

One proof of the Theorem uses alternants; the other uses the

“semi-skew Cauchy identity” X

λ∈Par

sλ(x)sλ/µ(y) =sµ(x)·

Y

i,j=1

(1−xiyj)−1

=sµ(x)· X

λ∈Par

hλ(x)mλ(y) (for any µ∈Par and for two sets of indeterminates x = (x1,x2,x3, . . .) and y = (y1,y2,y3, . . .)).

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(50)

Expanding Petries in the Schur basis: the formula

Theorem: Let k be a positive integer. Letµ∈Par. Then, G(k)·sµ= X

λ∈Par

petk(λ, µ)sλ. Thus, for each m∈N, we have

G(k,m)·sµ= X

λ∈Parm+|µ|

petk(λ, µ)sλ. Corollary: Let k be a positive integer. Then,

G(k) = X

λ∈Par

petk(λ,∅)sλ. Thus, for each m∈N, we have

G(k,m) = X

λ∈Parm

petk(λ,∅)sλ.

One proof of the Theorem uses alternants; the other uses the

“semi-skew Cauchy identity”

X

λ∈Par

sλ(x)sλ/µ(y) =sµ(x)·

Y

i,j=1

(1−xiyj)−1

=sµ(x)· X

λ∈Par

hλ(x)mλ(y) (for any µ∈Par and for two sets of indeterminates x = (x1,x2,x3, . . .) and y = (y1,y2,y3, . . .)).

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Expanding Petries in the Schur basis: the formula

Theorem: Let k be a positive integer. Letµ∈Par. Then, G(k)·sµ= X

λ∈Par

petk(λ, µ)sλ. Thus, for each m∈N, we have

G(k,m)·sµ= X

λ∈Parm+|µ|

petk(λ, µ)sλ.

One proof of the Theorem uses alternants; the other uses the

“semi-skew Cauchy identity”

X

λ∈Par

sλ(x)sλ/µ(y) =sµ(x)·

Y

i,j=1

(1−xiyj)−1

=sµ(x)· X

λ∈Par

hλ(x)mλ(y) (for any µ∈Par and for two sets of indeterminates x = (x1,x2,x3, . . .) and y = (y1,y2,y3, . . .)).

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What are the Petrie numbers?

We have shown that petk(λ, µ)∈ {0,1,−1}, but what exactly is it?

Gordon and Wilkinson 1974 prove that Petrie matrices have determinants ∈ {0,1,−1}by induction. This is little help to us.

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What are the Petrie numbers?

We have shown that petk(λ, µ)∈ {0,1,−1}, but what exactly is it?

Gordon and Wilkinson 1974prove that Petrie matrices have determinants ∈ {0,1,−1}by induction. This is little help to us.

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What are the Petrie numbers? The easy case

Proposition: Letλ∈Par and k >0 be such that λ1 ≥k. Then, petk(λ,∅) = 0.

To get a description in all other cases, recall the definition of transpose (aka conjugate) partitions:

Given a partition λ∈Par, we define the transpose partitionλt of λto be the partitionµ given by

µi =|{j ∈ {1,2,3, . . .} | λj ≥i}| for all i ≥1.

In terms of Young diagrams, this is just flipping the diagram of λacross the diagonal.

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What are the Petrie numbers? The easy case

Proposition: Letλ∈Par and k >0 be such that λ1 ≥k. Then, petk(λ,∅) = 0.

To get a description in all other cases, recall the definition of transpose (aka conjugate) partitions:

Given a partition λ∈Par, we define the transpose partitionλt of λto be the partitionµ given by

µi =|{j ∈ {1,2,3, . . .} | λj ≥i}| for all i ≥1.

In terms of Young diagrams, this is just flipping the diagram of λacross the diagonal.

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What are the Petrie numbers? Formula for petk(λ,∅) Theorem: Let λ∈Par and k >0 be such that λ1<k. Let µ=λt (the transpose partition of λ). Thus, µk = 0.

For eachi ∈ {1,2, . . . ,k−1}, set

βii−i and γi = 1 + (βi −1) %k

| {z }

remainder ofβi−1 modulok

.

(a)If thek−1 numbersγ1, γ2, . . . , γk−1 are not distinct, then petk(λ,∅) = 0.

(b) If thek−1 numbersγ1, γ2, . . . , γk−1 are distinct, then petk(λ,∅) = (−1)12+···+βk−1)+g+(γ12+···+γk−1), where

g = n

(i,j)∈ {1,2, . . . ,k−1}2 | i <j andγi < γjo . Question: Is there such a description for petk(λ, µ) ?

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What are the Petrie numbers? Formula for petk(λ,∅) Theorem: Let λ∈Par and k >0 be such that λ1<k. Let µ=λt (the transpose partition of λ). Thus, µk = 0.

For eachi ∈ {1,2, . . . ,k−1}, set

βii−i and γi = 1 + (βi −1) %k

| {z }

remainder ofβi−1 modulok

.

(a)If thek−1 numbersγ1, γ2, . . . , γk−1 are not distinct, then petk(λ,∅) = 0.

(b) If thek−1 numbersγ1, γ2, . . . , γk−1 are distinct, then petk(λ,∅) = (−1)12+···+βk−1)+g+(γ12+···+γk−1), where

g = n

(i,j)∈ {1,2, . . . ,k−1}2 | i <j andγi < γjo . Question: Is there such a description for petk(λ, µ) ?

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Other properties

For anyk >0, we define a map fk : Λ→Λ by setting fk(a) =a

x1k,x2k,x3k, . . .

for eacha∈Λ.

This map fk is called the k-th Frobenius endomorphismof Λ.

(Also known as plethysm bypk. Perhaps the nicest plethysm!) Theorem: Let k be a positive integer. Letm∈N. Then,

G(k,m) =X

i∈N

(−1)ihm−ki ·fk(ei).

Theorem: Fix a positive integerk. Assume that 1−k is invertible in k. Then, the family

(G(k,m))m≥1 = (G(k,1),G(k,2),G(k,3), . . .) is an algebraically independent generating set of the commutative k-algebra Λ.

Thus, products of several elements of this family form a basis of Λ (if 1−k is invertible in k). These bases remain to be studied.

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Other properties

For anyk >0, we define a map fk : Λ→Λ by setting fk(a) =a

x1k,x2k,x3k, . . .

for eacha∈Λ.

This map fk is called the k-th Frobenius endomorphismof Λ.

(Also known as plethysm bypk. Perhaps the nicest plethysm!) Theorem: Let k be a positive integer. Letm∈N. Then,

G(k,m) =X

i∈N

(−1)ihm−ki ·fk(ei).

Theorem: Fix a positive integerk. Assume that 1−k is invertible in k. Then, the family

(G(k,m))m≥1 = (G(k,1),G(k,2),G(k,3), . . .) is an algebraically independent generating set of the commutative k-algebra Λ.

Thus, products of several elements of this family form a basis of Λ (if 1−k is invertible in k). These bases remain to be studied.

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Other properties

For anyk >0, we define a map fk : Λ→Λ by setting fk(a) =a

x1k,x2k,x3k, . . .

for eacha∈Λ.

This map fk is called the k-th Frobenius endomorphismof Λ.

(Also known as plethysm bypk. Perhaps the nicest plethysm!) Theorem: Let k be a positive integer. Letm∈N. Then,

G(k,m) =X

i∈N

(−1)ihm−ki ·fk(ei).

Theorem: Fix a positive integerk. Assume that 1−k is invertible in k. Then, the family

(G(k,m))m≥1 = (G(k,1),G(k,2),G(k,3), . . .) is an algebraically independent generating set of the commutative k-algebra Λ.

Thus, products of several elements of this family form a basis of Λ (if 1−k is invertible in k). These bases remain to be studied.

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The Liu–Polo conjecture

This all begin with the following conjecture (Liu and Polo, arXiv:1908.08432):

X

λ∈Par2n−1; (n−1,n−1,1).λ

mλ =

n−2

X

i=0

(−1)is(n−1,n−1−i,1i+1) for anyn >1.

Here, the symbol. stands fordominance of partitions (also known as majorization); i.e., for two partitions λandµ, we have

λ . µ if and only if

12+· · ·+λi ≥µ12+· · ·+µi for all i). Let me briefly outline how this conjecture can be proved.

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The Liu–Polo conjecture, proof: 1

The partitions λ∈Par2n−1 satisfying (n−1,n−1,1). λ are precisely the partitionsλ∈Par2n−1 satisfyingλi <n for all i.

Thus,

X

λ∈Par2n−1; (n−1,n−1,1).λ

mλ=G(n,2n−1).

So it remains to show that G(n,2n−1) =

n−2

X

i=0

(−1)is(n−1,n−1−i,1i+1).

The formula for petk(λ,∅) should be useful here, but the combinatorics is tortuous.

Instead, we can work algebraically:

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The Liu–Polo conjecture, proof: 1

The partitions λ∈Par2n−1 satisfying (n−1,n−1,1). λ are precisely the partitionsλ∈Par2n−1 satisfyingλi <n for all i.

Thus,

X

λ∈Par2n−1; (n−1,n−1,1).λ

mλ=G(n,2n−1).

So it remains to show that G(n,2n−1) =

n−2

X

i=0

(−1)is(n−1,n−1−i,1i+1).

The formula for petk(λ,∅) should be useful here, but the combinatorics is tortuous.

Instead, we can work algebraically:

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The Liu–Polo conjecture, proof: 1

The partitions λ∈Par2n−1 satisfying (n−1,n−1,1). λ are precisely the partitionsλ∈Par2n−1 satisfyingλi <n for all i.

Thus,

X

λ∈Par2n−1; (n−1,n−1,1).λ

mλ=G(n,2n−1).

So it remains to show that G(n,2n−1) =

n−2

X

i=0

(−1)is(n−1,n−1−i,1i+1).

The formula for petk(λ,∅) should be useful here, but the combinatorics is tortuous.

Instead, we can work algebraically:

23 / 43

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