Relations among partitions. II: Adjusting for one partition R. A. - - PowerPoint PPT Presentation

relations among partitions ii adjusting for one partition
SMART_READER_LITE
LIVE PREVIEW

Relations among partitions. II: Adjusting for one partition R. A. - - PowerPoint PPT Presentation

Relations among partitions. II: Adjusting for one partition R. A. Bailey University of St Andrews Combinatorics Seminar, Shanghai Jiao Tong University, November 2017 Bailey Relations among partitions 1/21 Abstract Two partitions with n and


slide-1
SLIDE 1

Relations among partitions. II: Adjusting for one partition

  • R. A. Bailey

University of St Andrews Combinatorics Seminar, Shanghai Jiao Tong University, November 2017

Bailey Relations among partitions 1/21

slide-2
SLIDE 2

Abstract

Two partitions with n and m parts respectively define an n × m incidence matrix between the two partitions.

Bailey Relations among partitions 2/21

slide-3
SLIDE 3

Abstract

Two partitions with n and m parts respectively define an n × m incidence matrix between the two partitions. I will give a few examples to show the statistical background, to motivate the idea of projecting onto the

  • rthogonal complement of the subspace defined by a partition,

which is known as adjusting for that partition. From this point of view, the usual notion of balance (in incomplete block designs) is just adjusted uniformity. I will say a little about balanced block designs.

Bailey Relations among partitions 2/21

slide-4
SLIDE 4

Abstract

Two partitions with n and m parts respectively define an n × m incidence matrix between the two partitions. I will give a few examples to show the statistical background, to motivate the idea of projecting onto the

  • rthogonal complement of the subspace defined by a partition,

which is known as adjusting for that partition. From this point of view, the usual notion of balance (in incomplete block designs) is just adjusted uniformity. I will say a little about balanced block designs. Similarly, two partitions have adjusted orthogonality with respect to a third partition if adjusting for the third partition makes something defined by the first two really zero. Ordinary orthogonality can be recast in this light. Adjusted orthogonality can also be defined in terms of matrices, or, more combinatorially, by counting various things.

Bailey Relations among partitions 2/21

slide-5
SLIDE 5

Outline

◮ Incidence matrix between two partitions. ◮ Some statistical background. ◮ Balanced block designs. ◮ Adjusted orthogonality.

Bailey Relations among partitions 3/21

slide-6
SLIDE 6

Outline

◮ Incidence matrix between two partitions. ◮ Some statistical background. ◮ Balanced block designs. ◮ Adjusted orthogonality.

Bailey Relations among partitions 3/21

slide-7
SLIDE 7

Two partitions: incidence matrix

The number of parts of partition F is denoted nF. XF is the M × nF matrix with entry 1 in row ω and column j if ω is in part j of F, and all other entries 0.

Definition

If F and G are partitions of Ω then the nF × nG incidence matrix NFG is defined by NFG = X⊤

F XG.

The entry in row i and column j is the size of the intersection of the i-th part of F with the j-th part of G.

Bailey Relations among partitions 4/21

slide-8
SLIDE 8

Example of an incidence matrix

The parts of G are columns: nG = 12 and kG = 3. The parts of L are letters; nL = 9 and kL = 4. A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

Bailey Relations among partitions 5/21

slide-9
SLIDE 9

Example of an incidence matrix

The parts of G are columns: nG = 12 and kG = 3. The parts of L are letters; nL = 9 and kL = 4. A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G NLG =               1 0 0 1 0 0 1 0 0 1 0 0 1 0 0 0 1 0 0 1 0 0 1 0 1 0 0 0 0 1 0 0 1 0 0 1 0 1 0 1 0 0 0 0 1 0 1 0 0 1 0 0 1 0 1 0 0 0 0 1 0 1 0 0 0 1 0 1 0 1 0 0 0 0 1 1 0 0 0 1 0 0 0 1 0 0 1 0 1 0 0 0 1 1 0 0 0 0 1 0 0 1 1 0 0 0 1 0              

Bailey Relations among partitions 5/21

slide-10
SLIDE 10

Example of an incidence matrix

The parts of G are columns: nG = 12 and kG = 3. The parts of L are letters; nL = 9 and kL = 4. A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G NLG =               1 0 0 1 0 0 1 0 0 1 0 0 1 0 0 0 1 0 0 1 0 0 1 0 1 0 0 0 0 1 0 0 1 0 0 1 0 1 0 1 0 0 0 0 1 0 1 0 0 1 0 0 1 0 1 0 0 0 0 1 0 1 0 0 0 1 0 1 0 1 0 0 0 0 1 1 0 0 0 1 0 0 0 1 0 0 1 0 1 0 0 0 1 1 0 0 0 0 1 0 0 1 1 0 0 0 1 0               NLGN⊤

LG = 4I + 1(J − I).

Bailey Relations among partitions 5/21

slide-11
SLIDE 11

Outline

◮ Incidence matrix between two partitions. ◮ Some statistical background. ◮ Balanced block designs. ◮ Adjusted orthogonality.

Bailey Relations among partitions 6/21

slide-12
SLIDE 12

Outline

◮ Incidence matrix between two partitions. ◮ Some statistical background. ◮ Balanced block designs. ◮ Adjusted orthogonality.

Bailey Relations among partitions 6/21

slide-13
SLIDE 13

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

Bailey Relations among partitions 7/21

slide-14
SLIDE 14

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ The underlying set has size 36 (vegetable patches).

Bailey Relations among partitions 7/21

slide-15
SLIDE 15

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ The underlying set has size 36 (vegetable patches). ◮ The partition D into districts has 4 parts of size 9.

Bailey Relations among partitions 7/21

slide-16
SLIDE 16

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ The underlying set has size 36 (vegetable patches). ◮ The partition D into districts has 4 parts of size 9. ◮ The partition G into gardens has 12 parts of size 3.

Bailey Relations among partitions 7/21

slide-17
SLIDE 17

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ The underlying set has size 36 (vegetable patches). ◮ The partition D into districts has 4 parts of size 9. ◮ The partition G into gardens has 12 parts of size 3. ◮ The partition L into letters (lettuce varieties) has 9 parts of

size 4.

Bailey Relations among partitions 7/21

slide-18
SLIDE 18

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ The underlying set has size 36 (vegetable patches). ◮ The partition D into districts has 4 parts of size 9. ◮ The partition G into gardens has 12 parts of size 3. ◮ The partition L into letters (lettuce varieties) has 9 parts of

size 4.

Bailey Relations among partitions 7/21

slide-19
SLIDE 19

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ The underlying set has size 36 (vegetable patches). ◮ The partition D into districts has 4 parts of size 9. ◮ The partition G into gardens has 12 parts of size 3. ◮ The partition L into letters (lettuce varieties) has 9 parts of

size 4. Three binary relations:

◮ G ≺ D,

G is a refinement of D;

Bailey Relations among partitions 7/21

slide-20
SLIDE 20

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ The underlying set has size 36 (vegetable patches). ◮ The partition D into districts has 4 parts of size 9. ◮ The partition G into gardens has 12 parts of size 3. ◮ The partition L into letters (lettuce varieties) has 9 parts of

size 4. Three binary relations:

◮ G ≺ D,

G is a refinement of D;

◮ L⊥D,

L is strictly orthogonal to D;

Bailey Relations among partitions 7/21

slide-21
SLIDE 21

An example of three uniform partitions of the same set

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ The underlying set has size 36 (vegetable patches). ◮ The partition D into districts has 4 parts of size 9. ◮ The partition G into gardens has 12 parts of size 3. ◮ The partition L into letters (lettuce varieties) has 9 parts of

size 4. Three binary relations:

◮ G ≺ D,

G is a refinement of D;

◮ L⊥D,

L is strictly orthogonal to D;

◮ L ⊲ G,

L is balanced with respect to G.

Bailey Relations among partitions 7/21

slide-22
SLIDE 22

Why orthogonal projection? Back to gardening experiment

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ 12 gardens, each containing three vegetable patches; ◮ 9 lettuce varieties, each grown on four patches.

Bailey Relations among partitions 8/21

slide-23
SLIDE 23

Why orthogonal projection? Back to gardening experiment

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ 12 gardens, each containing three vegetable patches; ◮ 9 lettuce varieties, each grown on four patches.

Denote by Yω the total yield of edible lettuce on patch ω.

Bailey Relations among partitions 8/21

slide-24
SLIDE 24

Why orthogonal projection? Back to gardening experiment

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ 12 gardens, each containing three vegetable patches; ◮ 9 lettuce varieties, each grown on four patches.

Denote by Yω the total yield of edible lettuce on patch ω. Assume that Yω is a random variable with expectation τL(ω) + βG(ω).

Bailey Relations among partitions 8/21

slide-25
SLIDE 25

Why orthogonal projection? Back to gardening experiment

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ 12 gardens, each containing three vegetable patches; ◮ 9 lettuce varieties, each grown on four patches.

Denote by Yω the total yield of edible lettuce on patch ω. Assume that Yω is a random variable with expectation τL(ω) + βG(ω). I could add 51 to each τi and subtract 51 from each βj without changing this.

Bailey Relations among partitions 8/21

slide-26
SLIDE 26

Why orthogonal projection? Back to gardening experiment

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ 12 gardens, each containing three vegetable patches; ◮ 9 lettuce varieties, each grown on four patches.

Denote by Yω the total yield of edible lettuce on patch ω. Assume that Yω is a random variable with expectation τL(ω) + βG(ω). I could add 51 to each τi and subtract 51 from each βj without changing this. I would like to estimate τ1, . . . , τ9 up to an additive constant.

Bailey Relations among partitions 8/21

slide-27
SLIDE 27

Why orthogonal projection? Back to gardening experiment

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ 12 gardens, each containing three vegetable patches; ◮ 9 lettuce varieties, each grown on four patches.

Denote by Yω the total yield of edible lettuce on patch ω. Assume that Yω is a random variable with expectation τL(ω) + βG(ω). I could add 51 to each τi and subtract 51 from each βj without changing this. I would like to estimate τ1, . . . , τ9 up to an additive constant. I do not care about β1,. . . , β12.

Bailey Relations among partitions 8/21

slide-28
SLIDE 28

Why orthogonal projection? Back to gardening experiment

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ 12 gardens, each containing three vegetable patches; ◮ 9 lettuce varieties, each grown on four patches.

Denote by Yω the total yield of edible lettuce on patch ω. Assume that Yω is a random variable with expectation τL(ω) + βG(ω). I could add 51 to each τi and subtract 51 from each βj without changing this. I would like to estimate τ1, . . . , τ9 up to an additive constant. I do not care about β1,. . . , β12. So I put the responses Yω into a vector Y and project it onto V⊥

G .

Bailey Relations among partitions 8/21

slide-29
SLIDE 29

Why orthogonal projection? Back to gardening experiment

A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G

◮ 12 gardens, each containing three vegetable patches; ◮ 9 lettuce varieties, each grown on four patches.

Denote by Yω the total yield of edible lettuce on patch ω. Assume that Yω is a random variable with expectation τL(ω) + βG(ω). I could add 51 to each τi and subtract 51 from each βj without changing this. I would like to estimate τ1, . . . , τ9 up to an additive constant. I do not care about β1,. . . , β12. So I put the responses Yω into a vector Y and project it onto V⊥

G .

There are no βj in the expectation of (I − PG)Y.

Bailey Relations among partitions 8/21

slide-30
SLIDE 30

Outline

◮ Incidence matrix between two partitions. ◮ Some statistical background. ◮ Balanced block designs. ◮ Adjusted orthogonality.

Bailey Relations among partitions 9/21

slide-31
SLIDE 31

Outline

◮ Incidence matrix between two partitions. ◮ Some statistical background. ◮ Balanced block designs. ◮ Adjusted orthogonality.

Bailey Relations among partitions 9/21

slide-32
SLIDE 32

Balance as adjusted uniformity

NFG = X⊤

F XG = N⊤ GF

PB = 1

kB XBX⊤ B

What happens to properties of a single partition L when we project onto the orthogonal complement of the subspace VB defined by partition B?

Bailey Relations among partitions 10/21

slide-33
SLIDE 33

Balance as adjusted uniformity

NFG = X⊤

F XG = N⊤ GF

PB = 1

kB XBX⊤ B

What happens to properties of a single partition L when we project onto the orthogonal complement of the subspace VB defined by partition B? Partition L is uniform means that X⊤

L XL = NLL = diagonal matrix of sizes of parts of L

is a (non-zero) multiple of the identity matrix I of order nL. This is a special case of a completely symmetric matrix (a linear combination of I and the all-1 matrix J).

Bailey Relations among partitions 10/21

slide-34
SLIDE 34

Balance as adjusted uniformity

NFG = X⊤

F XG = N⊤ GF

PB = 1

kB XBX⊤ B

What happens to properties of a single partition L when we project onto the orthogonal complement of the subspace VB defined by partition B? Partition L is uniform means that X⊤

L XL = NLL = diagonal matrix of sizes of parts of L

is a (non-zero) multiple of the identity matrix I of order nL. This is a special case of a completely symmetric matrix (a linear combination of I and the all-1 matrix J). So to say that L has adjusted uniformity with respect to partition B should mean that X⊤

L (I − PB)XL is completely symmetric but not zero.

Bailey Relations among partitions 10/21

slide-35
SLIDE 35

Balance as adjusted uniformity

NFG = X⊤

F XG = N⊤ GF

PB = 1

kB XBX⊤ B

What happens to properties of a single partition L when we project onto the orthogonal complement of the subspace VB defined by partition B? Partition L is uniform means that X⊤

L XL = NLL = diagonal matrix of sizes of parts of L

is a (non-zero) multiple of the identity matrix I of order nL. This is a special case of a completely symmetric matrix (a linear combination of I and the all-1 matrix J). So to say that L has adjusted uniformity with respect to partition B should mean that X⊤

L (I − PB)XL is completely symmetric but not zero.

But X⊤

L (I − PB)XL = X⊤ L XL − 1 kB X⊤ L XBX⊤ B XL = NLL − 1 kB NLBNBL.

Bailey Relations among partitions 10/21

slide-36
SLIDE 36

Balance

Definition

Let L and B be uniform partitions of Ω. Then L is balanced with respect to B if X⊤

L (I − PB)XL = NLL − 1 kB NLBNBL is completely

symmetric but not zero.

Bailey Relations among partitions 11/21

slide-37
SLIDE 37

Balance

Definition

Let L and B be uniform partitions of Ω. Then L is balanced with respect to B if X⊤

L (I − PB)XL = NLL − 1 kB NLBNBL is completely

symmetric but not zero.

◮ ‘Non-zero’ excludes B L but does not exclude B⊥L.

Bailey Relations among partitions 11/21

slide-38
SLIDE 38

Balance

Definition

Let L and B be uniform partitions of Ω. Then L is balanced with respect to B if X⊤

L (I − PB)XL = NLL − 1 kB NLBNBL is completely

symmetric but not zero.

◮ ‘Non-zero’ excludes B L but does not exclude B⊥L. ◮ The (i, j)-entry of NLBNBL is the number of times that

letters i and j concur in blocks (allowing for multiplicities).

Bailey Relations among partitions 11/21

slide-39
SLIDE 39

Balance

Definition

Let L and B be uniform partitions of Ω. Then L is balanced with respect to B if X⊤

L (I − PB)XL = NLL − 1 kB NLBNBL is completely

symmetric but not zero.

◮ ‘Non-zero’ excludes B L but does not exclude B⊥L. ◮ The (i, j)-entry of NLBNBL is the number of times that

letters i and j concur in blocks (allowing for multiplicities).

◮ Statisticians always call this property ‘balance’,

but some of you may say that the parts of L and B form the points and blocks of a 2-design.

Bailey Relations among partitions 11/21

slide-40
SLIDE 40

Balance

Definition

Let L and B be uniform partitions of Ω. Then L is balanced with respect to B if X⊤

L (I − PB)XL = NLL − 1 kB NLBNBL is completely

symmetric but not zero.

◮ ‘Non-zero’ excludes B L but does not exclude B⊥L. ◮ The (i, j)-entry of NLBNBL is the number of times that

letters i and j concur in blocks (allowing for multiplicities).

◮ Statisticians always call this property ‘balance’,

but some of you may say that the parts of L and B form the points and blocks of a 2-design.

Bailey Relations among partitions 11/21

slide-41
SLIDE 41

Balance

Definition

Let L and B be uniform partitions of Ω. Then L is balanced with respect to B if X⊤

L (I − PB)XL = NLL − 1 kB NLBNBL is completely

symmetric but not zero.

◮ ‘Non-zero’ excludes B L but does not exclude B⊥L. ◮ The (i, j)-entry of NLBNBL is the number of times that

letters i and j concur in blocks (allowing for multiplicities).

◮ Statisticians always call this property ‘balance’,

but some of you may say that the parts of L and B form the points and blocks of a 2-design.

Definition

The relationship between L and B is binary if all parts of L ∧ B are singletons; it is generalized binary if every part of L meets every part of B and no pair of parts of L ∧ B have sizes differing by more than one.

Bailey Relations among partitions 11/21

slide-42
SLIDE 42

Fisher’s Inequality and related results

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B then nB ≥ nL.

Bailey Relations among partitions 12/21

slide-43
SLIDE 43

Fisher’s Inequality and related results

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B then nB ≥ nL.

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B and nB = nL, then B is balanced with respect to L.

Bailey Relations among partitions 12/21

slide-44
SLIDE 44

Fisher’s Inequality and related results

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B then nB ≥ nL.

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B and nB = nL, then B is balanced with respect to L.

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B then PL(VB) = VL.

Bailey Relations among partitions 12/21

slide-45
SLIDE 45

Fisher’s Inequality and related results

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B then nB ≥ nL.

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B and nB = nL, then B is balanced with respect to L.

Theorem

If L is balanced with respect to B but L is not strictly orthogonal to B then PL(VB) = VL. The proofs are a combination of counting arguments with the fact that the rank of the incidence matrix NLB cannot be greater than nL or nB.

Bailey Relations among partitions 12/21

slide-46
SLIDE 46

Balance, continued

Write L ◮ B if L is balanced with respect to B but L is not strictly orthogonal to B.

Bailey Relations among partitions 13/21

slide-47
SLIDE 47

Balance, continued

Write L ◮ B if L is balanced with respect to B but L is not strictly orthogonal to B. Write L ⊲ B if L ◮ B and the relationship beween L and B is (generalized) binary.

Bailey Relations among partitions 13/21

slide-48
SLIDE 48

Balance, continued

Write L ◮ B if L is balanced with respect to B but L is not strictly orthogonal to B. Write L ⊲ B if L ◮ B and the relationship beween L and B is (generalized) binary. Write L ⊲ ⊳ B if L ⊲ B and B ⊲ L.

Bailey Relations among partitions 13/21

slide-49
SLIDE 49

Balance, continued

Write L ◮ B if L is balanced with respect to B but L is not strictly orthogonal to B. Write L ⊲ B if L ◮ B and the relationship beween L and B is (generalized) binary. Write L ⊲ ⊳ B if L ⊲ B and B ⊲ L. If the relationship between L and B is binary and L ⊲ ⊳ B, then we have a symmetric balanced incomplete-block design.

Bailey Relations among partitions 13/21

slide-50
SLIDE 50

Balance, continued

Write L ◮ B if L is balanced with respect to B but L is not strictly orthogonal to B. Write L ⊲ B if L ◮ B and the relationship beween L and B is (generalized) binary. Write L ⊲ ⊳ B if L ⊲ B and B ⊲ L. If the relationship between L and B is binary and L ⊲ ⊳ B, then we have a symmetric balanced incomplete-block design. A B C D E F G H I A D G B E H C F I A E I B F G C D H A F H B D I C E G In the gardening experiment, L ⊲ G and the relationship is binary.

Bailey Relations among partitions 13/21

slide-51
SLIDE 51

Two block designs in which letters are balanced with respect to blocks, which are represented by columns

A A B C D E F G B A B C D E F G C A B C D E F G D A B C D E F G E A B C D E F G F A B C D E F G G A B C D E F G A A C C D D E E B B D D E E F F C C E E F F G G D D F F G G A A E E G G A A B B F F A A B B C C G G B B C C D D (a) (b) (a) is generalized binary but not binary; (b) is neither binary nor generalized binary.

Bailey Relations among partitions 14/21

slide-52
SLIDE 52

Outline

◮ Incidence matrix between two partitions. ◮ Some statistical background. ◮ Balanced block designs. ◮ Adjusted orthogonality.

Bailey Relations among partitions 15/21

slide-53
SLIDE 53

Outline

◮ Incidence matrix between two partitions. ◮ Some statistical background. ◮ Balanced block designs. ◮ Adjusted orthogonality.

Bailey Relations among partitions 15/21

slide-54
SLIDE 54

Orthogonality: recap

P0 = projector onto space V0 of constant vectors. F⊥G means that (I − P0)(VF) ⊥ (I − P0)(VG); equivalently, X⊤

F (I − P0)XG = 0.

Bailey Relations among partitions 16/21

slide-55
SLIDE 55

Orthogonality: recap

P0 = projector onto space V0 of constant vectors. F⊥G means that (I − P0)(VF) ⊥ (I − P0)(VG); equivalently, X⊤

F (I − P0)XG = 0.

We could say that F is orthogonal to G after adjusting for the partition U with a single part.

Bailey Relations among partitions 16/21

slide-56
SLIDE 56

Orthogonality: recap

P0 = projector onto space V0 of constant vectors. F⊥G means that (I − P0)(VF) ⊥ (I − P0)(VG); equivalently, X⊤

F (I − P0)XG = 0.

We could say that F is orthogonal to G after adjusting for the partition U with a single part. F ⊥ G means that (I − PF∨G)(VF) ⊥ (I − PF∨G)(VG); equivalently, X⊤

F (I − PF∨G)XG = 0.

Bailey Relations among partitions 16/21

slide-57
SLIDE 57

Orthogonality: recap

P0 = projector onto space V0 of constant vectors. F⊥G means that (I − P0)(VF) ⊥ (I − P0)(VG); equivalently, X⊤

F (I − P0)XG = 0.

We could say that F is orthogonal to G after adjusting for the partition U with a single part. F ⊥ G means that (I − PF∨G)(VF) ⊥ (I − PF∨G)(VG); equivalently, X⊤

F (I − PF∨G)XG = 0.

We could say that F is orthogonal to G after adjusting for their supremum F ∨ G.

Bailey Relations among partitions 16/21

slide-58
SLIDE 58

Adjusted orthogonality

NRC = X⊤

R XC = nR × nC incidence matrix of R-parts with C-parts

Definition

Let R (rows), C (columns) and L (letters) be three partitions on a finite set Ω. Then R and C have adjusted orthogonality with respect to L if (I − PL)(VR) ⊥ (I − PL)(VC).

Bailey Relations among partitions 17/21

slide-59
SLIDE 59

Adjusted orthogonality

NRC = X⊤

R XC = nR × nC incidence matrix of R-parts with C-parts

Definition

Let R (rows), C (columns) and L (letters) be three partitions on a finite set Ω. Then R and C have adjusted orthogonality with respect to L if (I − PL)(VR) ⊥ (I − PL)(VC). Equivalent conditions Mode of thinking (I − PL)(VR) ⊥ (I − PL)(VC) angles between subspaces

Bailey Relations among partitions 17/21

slide-60
SLIDE 60

Adjusted orthogonality

NRC = X⊤

R XC = nR × nC incidence matrix of R-parts with C-parts

Definition

Let R (rows), C (columns) and L (letters) be three partitions on a finite set Ω. Then R and C have adjusted orthogonality with respect to L if (I − PL)(VR) ⊥ (I − PL)(VC). Equivalent conditions Mode of thinking (I − PL)(VR) ⊥ (I − PL)(VC) angles between subspaces X⊤

R (I − PL)XC = 0

matrix equation

Bailey Relations among partitions 17/21

slide-61
SLIDE 61

Adjusted orthogonality

NRC = X⊤

R XC = nR × nC incidence matrix of R-parts with C-parts

Definition

Let R (rows), C (columns) and L (letters) be three partitions on a finite set Ω. Then R and C have adjusted orthogonality with respect to L if (I − PL)(VR) ⊥ (I − PL)(VC). Equivalent conditions Mode of thinking (I − PL)(VR) ⊥ (I − PL)(VC) angles between subspaces X⊤

R (I − PL)XC = 0

matrix equation X⊤

R XC = X⊤ R PLXC

matrix equation

Bailey Relations among partitions 17/21

slide-62
SLIDE 62

Adjusted orthogonality

NRC = X⊤

R XC = nR × nC incidence matrix of R-parts with C-parts

Definition

Let R (rows), C (columns) and L (letters) be three partitions on a finite set Ω. Then R and C have adjusted orthogonality with respect to L if (I − PL)(VR) ⊥ (I − PL)(VC). Equivalent conditions Mode of thinking (I − PL)(VR) ⊥ (I − PL)(VC) angles between subspaces X⊤

R (I − PL)XC = 0

matrix equation X⊤

R XC = X⊤ R PLXC

matrix equation if L is uniform, kLNRC = NRLNLC counting equation

Bailey Relations among partitions 17/21

slide-63
SLIDE 63

Adjusted orthogonality

NRC = X⊤

R XC = nR × nC incidence matrix of R-parts with C-parts

Definition

Let R (rows), C (columns) and L (letters) be three partitions on a finite set Ω. Then R and C have adjusted orthogonality with respect to L if (I − PL)(VR) ⊥ (I − PL)(VC). Equivalent conditions Mode of thinking (I − PL)(VR) ⊥ (I − PL)(VC) angles between subspaces X⊤

R (I − PL)XC = 0

matrix equation X⊤

R XC = X⊤ R PLXC

matrix equation if L is uniform, kLNRC = NRLNLC counting equation The number of letters in common to row i and column j is kL × |row i ∩ column j| .

Bailey Relations among partitions 17/21

slide-64
SLIDE 64

A nasty example of adjusted orthogonality (Preece, 1988)

A F D G J C D B G E H F G E C H A I J H A D I B C F I B E J

◮ |Ω| = 30; ◮ 5 rows, each of size 6; ◮ 5 columns, each of size 6; ◮ 10 letters, each of “size” 3.

The number of letters in common to row i and column j is

  • 6

if i = j 3

  • therwise.

Bailey Relations among partitions 18/21

slide-65
SLIDE 65

A nicer example of adjusted orthogonality

H J I G F E J I H C B D D F A J G C A B G E D I E A C B H F

◮ |Ω| = 30; ◮ 5 rows, each of size 6; ◮ 6 columns, each of size 5; ◮ 10 letters, each of “size” 3.

The number of letters in common to row i and column j is always 3.

Bailey Relations among partitions 19/21

slide-66
SLIDE 66

A nicer example of adjusted orthogonality

H J I G F E J I H C B D D F A J G C A B G E D I E A C B H F

◮ |Ω| = 30; ◮ 5 rows, each of size 6; ◮ 6 columns, each of size 5; ◮ 10 letters, each of “size” 3.

The number of letters in common to row i and column j is always 3. This is a consequence of adjusted orthogonality if R⊥C and R ∧ C is uniform.

Bailey Relations among partitions 19/21

slide-67
SLIDE 67

Possible uses for this design

H J I G F E J I H C B D D F A J G C A B G E D I E A C B H F An experiment to compare exercise regimes

◮ 5 months = 5 rows; ◮ 6 people = 6 columns; ◮ 10 exercise regimes = 10 letters; ◮ allocate exercise regimes to people-month combinations.

An experiment to compare lettuce varieties and watering regimes

◮ 5 watering regimes = 5 rows; ◮ 6 varieties of lettuce = 6 columns; ◮ 10 gardens = 10 letters; ◮ allocate lettuce-watering combinations to gardens.

Bailey Relations among partitions 20/21

slide-68
SLIDE 68

Some comments on the history

Agrawal (1966) and Preece (1966) introduced the general idea

  • f adjusted orthogonality in contemporaneous papers,

but they neither defined it nor named it.

Bailey Relations among partitions 21/21

slide-69
SLIDE 69

Some comments on the history

Agrawal (1966) and Preece (1966) introduced the general idea

  • f adjusted orthogonality in contemporaneous papers,

but they neither defined it nor named it. It had been previously used in isolated examples.

Bailey Relations among partitions 21/21

slide-70
SLIDE 70

Some comments on the history

Agrawal (1966) and Preece (1966) introduced the general idea

  • f adjusted orthogonality in contemporaneous papers,

but they neither defined it nor named it. It had been previously used in isolated examples. It was introduced, but not named, independently by several authors in the next decade.

Bailey Relations among partitions 21/21

slide-71
SLIDE 71

Some comments on the history

Agrawal (1966) and Preece (1966) introduced the general idea

  • f adjusted orthogonality in contemporaneous papers,

but they neither defined it nor named it. It had been previously used in isolated examples. It was introduced, but not named, independently by several authors in the next decade. Eccleston and Russell (1975) independently introduced the concept; they named it in a 1977 paper.

Bailey Relations among partitions 21/21

slide-72
SLIDE 72

Some comments on the history

Agrawal (1966) and Preece (1966) introduced the general idea

  • f adjusted orthogonality in contemporaneous papers,

but they neither defined it nor named it. It had been previously used in isolated examples. It was introduced, but not named, independently by several authors in the next decade. Eccleston and Russell (1975) independently introduced the concept; they named it in a 1977 paper. It took a while before adjusted orthogonality became the standard wording, so my BCC survey may have missed some references.

Bailey Relations among partitions 21/21

slide-73
SLIDE 73

Some comments on the history

Agrawal (1966) and Preece (1966) introduced the general idea

  • f adjusted orthogonality in contemporaneous papers,

but they neither defined it nor named it. It had been previously used in isolated examples. It was introduced, but not named, independently by several authors in the next decade. Eccleston and Russell (1975) independently introduced the concept; they named it in a 1977 paper. It took a while before adjusted orthogonality became the standard wording, so my BCC survey may have missed some references. Part of the difficulty may have been the three modes of thinking (angles between subspaces; matrix equations; a counting equation) about equivalent versions of the

  • definition. Some results are obvious in one mode of thinking

but not in the others.

Bailey Relations among partitions 21/21