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>
© Rendiconti del Seminario Matematico della Università di Padova, 1956, tous droits réservés.
L’accès aux archives de la revue « Rendiconti del Seminario Matematico della Università di Padova » (http://rendiconti.math.unipd.it/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions).
Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
Nota
(*)
di MAHADEB DUTTA ( c~Calcutta)
INTRODUCTION. - In recent
investigations
of statisticalphy- sics,
thetheory
ofpartition
of numbersplays
a veryimpor-
tant role.
Temperly ~)
and others have used methods ofparti-
tions of numbers with convenience and
advantage
in caseswhen the usual method of statistical
mechanics, viz.,
methodof
steepest descent,
does notyield
desired accuracy, or is not valid. In an essential statisticalapproach
tothermodynamic problems,
fromgeneral
statisticalconsiderations,
Dutta2)
hasobtained some
general
formulae from which different stati-stics, viz.,
those ofBose, Fermi, Gentile,
Maxwell-Boltzmanncan be deduced
by using
differentpartitions
of numbers. Thishas necessitated the introduction and a
thorough investigation
of a new
type
ofpartitions
of numbers in which therepetition
of any
part
of the number inpartition
is restrictedsuitably.
In the
existing theory,
unrestrictedpartitions
have beenextensively
andthoroughly investigated by Hardy
and Rama-nujan 3),
Rademacher4)
and many others. Someinvestigations 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& 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. & 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
139
have also been made of
partitions
of numbers inunequal parts,
these into
parts
notexceeding
agiven number,
and the like.Kothari and his associates
g)
have discussedpartitions
of num-bers
occurring
in statisticalphysics, viz., partition
in powers ofintegers,
that in oddmultiples
ofhalf,
and thelike, by
themethods of statistical
mechanics,
which areonly repetitions
of usual calculations of statistical mechanics
by dropping
thephysical interpretation
ofquantities
involved in those calcu- lations. But noattempt
hasyet
been made to define and toinvestigate partitions
of numbers in which therepetition
ofa
part
isrestricted, though
these are ofgreat importance
forapplications
in statisticalphysics.
Mathematicalproblems
ofstatistics of
Bose,
Gentile and Fermi are those ofpartitions
of numbers
(energy)
intoparts
in whichrepetiton
ofparts
are restricted
differently
.Inpartitions corresponding
to Bosestatistics any
part
can berepeated
any number oftimes,
thatto Gentile
statistics,
anypart
can berepeated upto
« d ~ timeswhere d is any fixed
number,
and that to Fermi statistics nopart
canrepeat,
i. e. d =1.In this
note,
apartition
of number in which anypart
canbe
repeated upto
c d 3, times has been introduced and its sim-ple algebraic properties
have beeninvestigated.
Arough
ap-proximate
value for thispartition
has been calculatedby
aTauberian theorem.
Evidently
the formulae forpartition
ofunequal parts
and unrestrictedpartition
are obtained when d = 1 and d - oorespectively.
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.
Definition and
investigation
ofsimple algebraic properties:
DEFINITION. - is the
partition
of a number ~V into any numberparts,
in which nopart
isrepeated
more than d times.The
generating
funtion thispartition
iswhere
p (rc)
is unrestrictedpartition.
Equating
co-efficients of like powers ofsn,
weget
141
Thus,
numerical values of can be calculated succes-sively
from values ofp (n)
and soultimately
from Euler’s table.Now,
fromgeneral
valuesof n,
whenrrz ( d ~--1 )
~ ~(w + -f- 1) (d -~-1),
theexpression
can also be written asIf 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 asThus,
the formula is establishedby
the secondprinciple
offinite induction
~).
An
approximate
valuationof dp(nj by a Tauberian Theorem :
An
approximate
value correctupto
theexponential
orderalone for for
large 11.
can bebery easily
obtainedby
thehelp
of a Tauberian theoremalready
usedby Hardy
and Ra-manujan 3).
The theorem is : .«If
power seriespositive co-effi-
cients and
then,
when n - oo >>.Here let
and
by
definition.Then,
1) Cf. e.g. : BIRKHOFF, G. and MAcLANE, S., A Survey of Modern aZgebra. ( 19a3 ) , p. 13.
143
i.e.
When
d = I,
When
The last two results for
partition
intaunequal parts
andunrestricted
partition
are inagreement
with theapproxi-
mate
expression
obtainedby Hardy
andRamanujan 3) upto
the
exponential
order.The result for unrestricted
partition
may be used to find out thedominating
term in theexpression
forentropy
ofthe
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.