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On new partition of numbers

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(1)

R ENDICONTI

del

S EMINARIO M ATEMATICO

della

U NIVERSITÀ DI P ADOVA

M AHADEB D UTTA

On new partition of numbers

Rendiconti del Seminario Matematico della Università di Padova, tome 25 (1956), p. 138-143

<http://www.numdam.org/item?id=RSMUP_1956__25__138_0>

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(2)

Nota

(*)

di MAHADEB DUTTA ( c~

Calcutta)

INTRODUCTION. - In recent

investigations

of statistical

phy- sics,

the

theory

of

partition

of numbers

plays

a very

impor-

tant role.

Temperly ~)

and others have used methods of

parti-

tions of numbers with convenience and

advantage

in cases

when the usual method of statistical

mechanics, viz.,

method

of

steepest descent,

does not

yield

desired accuracy, or is not valid. In an essential statistical

approach

to

thermodynamic problems,

from

general

statistical

considerations,

Dutta

2)

has

obtained some

general

formulae from which different stati-

stics, viz.,

those of

Bose, Fermi, Gentile,

Maxwell-Boltzmann

can be deduced

by using

different

partitions

of numbers. This

has necessitated the introduction and a

thorough investigation

of a new

type

of

partitions

of numbers in which the

repetition

of any

part

of the number in

partition

is restricted

suitably.

In the

existing theory,

unrestricted

partitions

have been

extensively

and

thoroughly investigated by Hardy

and Rama-

nujan 3),

Rademacher

4)

and many others. Some

investigations 5)

(~) Pcrveu1.Ita in Redazione il 24 ottobre 7 955.

Indirizzo dell’A.: College of Science, University, Calcutta (India).

1) TEMPEBLY, H. N. v., Statistical Mechanics and the Partition of Num-

b6r&#x26; I. The Transition of liquid Helium. Proc. Iloy Soc. Lond., 109, (1949), 361-375.

2) DurrA, M., An Essential Statistical Approach to Thermodynamic Proc. Nat. Inst. Sc. India, 19, (1935), 109-26.

DUTTA, M., An Es.8ential Statistical Approach to Thermodynamic Problein II. Proc. Nat. Inst. Sc. India, (in press).

3) HARDY, G. H. &#x26; RAMANU.IAN, S., Asymptotic Formula in Combi- natory Anatpsis. Procl, Lond. Math. Soc. (2), 17, (1918), 15-115, also

Collected Papers of S. Raumanujan, 276-309.

4) RADE, M_4.CHER H., A Convergent Series for the Partition Function p ( n ) , Proc. Nat. Acad. Sc., U.S.A. 23, (1937), 78-84.

) HUA, L. K., On the Number of Partitions of a Number into

(3)

139

have also been made of

partitions

of numbers in

unequal parts,

these into

parts

not

exceeding

a

given number,

and the like.

Kothari and his associates

g)

have discussed

partitions

of num-

bers

occurring

in statistical

physics, viz., partition

in powers of

integers,

that in odd

multiples

of

half,

and the

like, by

the

methods of statistical

mechanics,

which are

only repetitions

of usual calculations of statistical mechanics

by dropping

the

physical interpretation

of

quantities

involved in those calcu- lations. But no

attempt

has

yet

been made to define and to

investigate partitions

of numbers in which the

repetition

of

a

part

is

restricted, though

these are of

great importance

for

applications

in statistical

physics.

Mathematical

problems

of

statistics of

Bose,

Gentile and Fermi are those of

partitions

of numbers

(energy)

into

parts

in which

repetiton

of

parts

are restricted

differently

.In

partitions corresponding

to Bose

statistics any

part

can be

repeated

any number of

times,

that

to Gentile

statistics,

any

part

can be

repeated upto

« d ~ times

where d is any fixed

number,

and that to Fermi statistics no

part

can

repeat,

i. e. d =1.

In this

note,

a

partition

of number in which any

part

can

be

repeated upto

c d 3, times has been introduced and its sim-

ple algebraic properties

have been

investigated.

A

rough

ap-

proximate

value for this

partition

has been calculated

by

a

Tauberian theorem.

Evidently

the formulae for

partition

of

unequal parts

and unrestricted

partition

are obtained when d = 1 and d - oo

respectively.

Unequal Parts. Bull. Amer. Math. Soc. 49, (1940), 419, abs. No. 279.

E1mös, P and J., The Distribution of the Number of Sum-

niands in the Partitions of a positive Number. Duke Math. J., 8, (1941), 335-345.

Cst PTA, H., A Partition. J. Ind. Math. Soc. 6, (1942), 115-17.

) AUr;LCx, F. C. and KOTHARI, D. S., Statistical Mechanics an the Partitions of Number. Proc.- Camb. Phil. Soc. 42, (1946), 272-277.

AVLUCK, F. C. and KOTARI, D. S., Partitzons into Powers of Inte- gra,ls. Proc. Roy Irish Acad. Minutes of Proceedings, Session 1946- 1947, 13.

AULUCK, F. C., SINGWI, K. S. and AGARWALA, B. K., On a New type of Partitions. Proc. Nat. Inst. Sc. India, 16, (1950), 147-156.

(4)

Definition and

investigation

of

simple algebraic properties:

DEFINITION. - is the

partition

of a number ~V into any number

parts,

in which no

part

is

repeated

more than d times.

The

generating

funtion this

partition

is

where

p (rc)

is unrestricted

partition.

Equating

co-efficients of like powers of

sn,

we

get

(5)

141

Thus,

numerical values of can be calculated succes-

sively

from values of

p (n)

and so

ultimately

from Euler’s table.

Now,

from

general

values

of n,

when

rrz ( d ~--1 )

~ ~

(w + -f- 1) (d -~-1),

the

expression

can also be written as

If this formula is true for this n and all its

preceeding

values then the

expression for n,

where

(m -f-1) (d -~-1)

:!5;- n

( m + 2) ( d + 1),

follows as

(6)

Thus,

the formula is established

by

the second

principle

of

finite induction

~).

An

approximate

valuation

of dp(nj by a Tauberian Theorem :

An

approximate

value correct

upto

the

exponential

order

alone for for

large 11.

can be

bery easily

obtained

by

the

help

of a Tauberian theorem

already

used

by Hardy

and Ra-

manujan 3).

The theorem is : .

«If

power series

positive co-effi-

cients and

then,

when n - oo &#x3E;&#x3E;.

Here let

and

by

definition.

Then,

1) Cf. e.g. : BIRKHOFF, G. and MAcLANE, S., A Survey of Modern aZgebra. ( 19a3 ) , p. 13.

(7)

143

i.e.

When

d = I,

When

The last two results for

partition

inta

unequal parts

and

unrestricted

partition

are in

agreement

with the

approxi-

mate

expression

obtained

by Hardy

and

Ramanujan 3) upto

the

exponential

order.

The result for unrestricted

partition

may be used to find out the

dominating

term in the

expression

for

entropy

of

the

corresponding thermodynamic system.

This is-

important

for

applications.

The author desires to express his thanks to Prof. S. N.

Bose and Mr. P. K. Ghosh for the interest taken i~r this work.

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