Elliptic functions historically comprise the elliptic integrals and their inverses, and originate from the problem of computing the arc length of an ellipse. From a more modern point of view, an elliptic function is defined as a doubly periodic function, i.e. a function which satisfies
for some half-periods with
. The canonical elliptic
functions are the Jacobi elliptic functions. More broadly, this section
includes quasi-doubly periodic functions (such as the Jacobi theta
functions) and other functions useful in the study of elliptic functions.
Many different conventions for the arguments of
elliptic functions are in use. It is even standard to use
different parameterizations for different functions in the same
text or software (and mpmath is no exception).
The usual parameters are the elliptic nome , which usually
must satisfy
; the elliptic parameter
(an arbitrary
complex number); the elliptic modulus
(an arbitrary complex
number); and the half-period ratio
, which usually must
satisfy
.
These quantities can be expressed in terms of each other
using the following relations:
In addition, an alternative definition is used for the nome in number theory, which we here denote by q-bar:
For convenience, mpmath provides functions to convert between the various parameters (qfrom(), mfrom(), kfrom(), taufrom(), qbarfrom()).
References
Returns the elliptic nome , given any of
:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> qfrom(q=0.25)
0.25
>>> qfrom(m=mfrom(q=0.25))
0.25
>>> qfrom(k=kfrom(q=0.25))
0.25
>>> qfrom(tau=taufrom(q=0.25))
(0.25 + 0.0j)
>>> qfrom(qbar=qbarfrom(q=0.25))
0.25
Returns the number-theoretic nome , given any of
:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> qbarfrom(qbar=0.25)
0.25
>>> qbarfrom(q=qfrom(qbar=0.25))
0.25
>>> qbarfrom(m=extraprec(20)(mfrom)(qbar=0.25)) # ill-conditioned
0.25
>>> qbarfrom(k=extraprec(20)(kfrom)(qbar=0.25)) # ill-conditioned
0.25
>>> qbarfrom(tau=taufrom(qbar=0.25))
(0.25 + 0.0j)
Returns the elliptic parameter , given any of
:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> mfrom(m=0.25)
0.25
>>> mfrom(q=qfrom(m=0.25))
0.25
>>> mfrom(k=kfrom(m=0.25))
0.25
>>> mfrom(tau=taufrom(m=0.25))
(0.25 + 0.0j)
>>> mfrom(qbar=qbarfrom(m=0.25))
0.25
As and
,
rapidly approaches
and
respectively:
>>> mfrom(q=0.75)
0.9999999999999798332943533
>>> mfrom(q=-0.75)
-49586681013729.32611558353
>>> mfrom(q=1)
1.0
>>> mfrom(q=-1)
-inf
The inverse nome as a function of has an integer
Taylor series expansion:
>>> taylor(lambda q: mfrom(q), 0, 7)
[0.0, 16.0, -128.0, 704.0, -3072.0, 11488.0, -38400.0, 117632.0]
Returns the elliptic modulus , given any of
:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> kfrom(k=0.25)
0.25
>>> kfrom(m=mfrom(k=0.25))
0.25
>>> kfrom(q=qfrom(k=0.25))
0.25
>>> kfrom(tau=taufrom(k=0.25))
(0.25 + 0.0j)
>>> kfrom(qbar=qbarfrom(k=0.25))
0.25
As and
,
rapidly approaches
and
respectively:
>>> kfrom(q=0.75)
0.9999999999999899166471767
>>> kfrom(q=-0.75)
(0.0 + 7041781.096692038332790615j)
>>> kfrom(q=1)
1
>>> kfrom(q=-1)
(0.0 + +infj)
Returns the elliptic half-period ratio , given any of
:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> taufrom(tau=0.5j)
(0.0 + 0.5j)
>>> taufrom(q=qfrom(tau=0.5j))
(0.0 + 0.5j)
>>> taufrom(m=mfrom(tau=0.5j))
(0.0 + 0.5j)
>>> taufrom(k=kfrom(tau=0.5j))
(0.0 + 0.5j)
>>> taufrom(qbar=qbarfrom(tau=0.5j))
(0.0 + 0.5j)
Evaluates the complete elliptic integral of the first kind,
, defined by
Note that the argument is the parameter ,
not the modulus
which is sometimes used.
Alternatively, in terms of a hypergeometric function, we have:
Examples
Values and limits include:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> ellipk(0)
1.570796326794896619231322
>>> ellipk(inf)
(0.0 + 0.0j)
>>> ellipk(-inf)
0.0
>>> ellipk(1)
+inf
>>> ellipk(-1)
1.31102877714605990523242
>>> ellipk(2)
(1.31102877714605990523242 - 1.31102877714605990523242j)
Verifying the defining integral and hypergeometric representation:
>>> ellipk(0.5)
1.85407467730137191843385
>>> quad(lambda t: (1-0.5*sin(t)**2)**-0.5, [0, pi/2])
1.85407467730137191843385
>>> pi/2*hyp2f1(0.5,0.5,1,0.5)
1.85407467730137191843385
Evaluation is supported for arbitrary complex :
>>> ellipk(3+4j)
(0.9111955638049650086562171 + 0.6313342832413452438845091j)
A definite integral:
>>> quad(ellipk, [0, 1])
2.0
Evaluates the complete elliptic integral of the second kind,
, defined by
Note that the argument is the parameter ,
not the modulus
which is sometimes used.
Alternatively, in terms of a hypergeometric function, we have:
Examples
Basic values and limits:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> ellipe(0)
1.570796326794896619231322
>>> ellipe(1)
1.0
>>> ellipe(-1)
1.910098894513856008952381
>>> ellipe(2)
(0.5990701173677961037199612 + 0.5990701173677961037199612j)
>>> ellipe(inf)
(0.0 + +infj)
>>> ellipe(-inf)
+inf
Verifying the defining integral and hypergeometric representation:
>>> ellipe(0.5)
1.350643881047675502520175
>>> quad(lambda t: sqrt(1-0.5*sin(t)**2), [0, pi/2])
1.350643881047675502520175
>>> pi/2*hyp2f1(0.5,-0.5,1,0.5)
1.350643881047675502520175
Evaluation is supported for arbitrary complex :
>>> ellipe(0.5+0.25j)
(1.360868682163129682716687 - 0.1238733442561786843557315j)
>>> ellipe(3+4j)
(1.499553520933346954333612 - 1.577879007912758274533309j)
A definite integral:
>>> quad(ellipe, [0,1])
1.333333333333333333333333
Computes the Jacobi theta function , where
, defined by the infinite series:
The theta functions are functions of two variables:
The compact notations
and
are also frequently
encountered. Finally, Jacobi theta functions are frequently
considered as functions of the half-period ratio
and then usually denoted by
.
Optionally, jtheta(n, z, q, derivative=d) with computes
a
-th derivative with respect to
.
Examples and basic properties
Considered as functions of , the Jacobi theta functions may be
viewed as generalizations of the ordinary trigonometric functions
cos and sin. They are periodic functions:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> jtheta(1, 0.25, '0.2')
0.2945120798627300045053104
>>> jtheta(1, 0.25 + 2*pi, '0.2')
0.2945120798627300045053104
Indeed, the series defining the theta functions are essentially trigonometric Fourier series. The coefficients can be retrieved using fourier():
>>> mp.dps = 10
>>> nprint(fourier(lambda x: jtheta(2, x, 0.5), [-pi, pi], 4))
([0.0, 1.68179, 0.0, 0.420448, 0.0], [0.0, 0.0, 0.0, 0.0, 0.0])
The Jacobi theta functions are also so-called quasiperiodic
functions of and
, meaning that for fixed
,
and
are the same
except for an exponential factor:
>>> mp.dps = 25
>>> tau = 3*j/10
>>> q = exp(pi*j*tau)
>>> z = 10
>>> jtheta(4, z+tau*pi, q)
(-0.682420280786034687520568 + 1.526683999721399103332021j)
>>> -exp(-2*j*z)/q * jtheta(4, z, q)
(-0.682420280786034687520568 + 1.526683999721399103332021j)
The Jacobi theta functions satisfy a huge number of other
functional equations, such as the following identity (valid for
any ):
>>> q = mpf(3)/10
>>> jtheta(3,0,q)**4
6.823744089352763305137427
>>> jtheta(2,0,q)**4 + jtheta(4,0,q)**4
6.823744089352763305137427
Extensive listings of identities satisfied by the Jacobi theta functions can be found in standard reference works.
The Jacobi theta functions are related to the gamma function for special arguments:
>>> jtheta(3, 0, exp(-pi))
1.086434811213308014575316
>>> pi**(1/4.) / gamma(3/4.)
1.086434811213308014575316
jtheta() supports arbitrary precision evaluation and complex arguments:
>>> mp.dps = 50
>>> jtheta(4, sqrt(2), 0.5)
2.0549510717571539127004115835148878097035750653737
>>> mp.dps = 25
>>> jtheta(4, 1+2j, (1+j)/5)
(7.180331760146805926356634 - 1.634292858119162417301683j)
Evaluation of derivatives:
>>> mp.dps = 25
>>> jtheta(1, 7, 0.25, 1); diff(lambda z: jtheta(1, z, 0.25), 7)
1.209857192844475388637236
1.209857192844475388637236
>>> jtheta(1, 7, 0.25, 2); diff(lambda z: jtheta(1, z, 0.25), 7, 2)
-0.2598718791650217206533052
-0.2598718791650217206533052
>>> jtheta(2, 7, 0.25, 1); diff(lambda z: jtheta(2, z, 0.25), 7)
-1.150231437070259644461474
-1.150231437070259644461474
>>> jtheta(2, 7, 0.25, 2); diff(lambda z: jtheta(2, z, 0.25), 7, 2)
-0.6226636990043777445898114
-0.6226636990043777445898114
>>> jtheta(3, 7, 0.25, 1); diff(lambda z: jtheta(3, z, 0.25), 7)
-0.9990312046096634316587882
-0.9990312046096634316587882
>>> jtheta(3, 7, 0.25, 2); diff(lambda z: jtheta(3, z, 0.25), 7, 2)
-0.1530388693066334936151174
-0.1530388693066334936151174
>>> jtheta(4, 7, 0.25, 1); diff(lambda z: jtheta(4, z, 0.25), 7)
0.9820995967262793943571139
0.9820995967262793943571139
>>> jtheta(4, 7, 0.25, 2); diff(lambda z: jtheta(4, z, 0.25), 7, 2)
0.3936902850291437081667755
0.3936902850291437081667755
Possible issues
For or
, jtheta() raises
ValueError. This exception is also raised for
extremely
close to 1 (or equivalently
very close to 0), since the
series would converge too slowly:
>>> jtheta(1, 10, 0.99999999 * exp(0.5*j))
Traceback (most recent call last):
...
ValueError: abs(q) > THETA_Q_LIM = 1.000000
Computes any of the Jacobi elliptic functions, defined in terms of Jacobi theta functions as
or more generally computes a ratio of two such functions. Here
, and
denotes the nome (see
nome()). Optionally, you can specify the nome directly
instead of
by passing q=<value>, or you can directly
specify the elliptic parameter
with k=<value>.
The first argument should be a two-character string specifying the
function using any combination of 's', 'c', 'd', 'n'. These
letters respectively denote the basic functions
,
,
, and
.
The identifier specifies the ratio of two such functions.
For example, 'ns' identifies the function
and 'cd' identifies the function
If called with only the first argument, a function object evaluating the chosen function for given arguments is returned.
Examples
Basic evaluation:
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> ellipfun('cd', 3.5, 0.5)
-0.9891101840595543931308394
>>> ellipfun('cd', 3.5, q=0.25)
0.07111979240214668158441418
The sn-function is doubly periodic in the complex plane with periods
and
(see ellipk()):
>>> sn = ellipfun('sn')
>>> sn(2, 0.25)
0.9628981775982774425751399
>>> sn(2+4*ellipk(0.25), 0.25)
0.9628981775982774425751399
>>> chop(sn(2+2*j*ellipk(1-0.25), 0.25))
0.9628981775982774425751399
The cn-function is doubly periodic with periods and
:
>>> cn = ellipfun('cn')
>>> cn(2, 0.25)
-0.2698649654510865792581416
>>> cn(2+4*ellipk(0.25), 0.25)
-0.2698649654510865792581416
>>> chop(cn(2+4*j*ellipk(1-0.25), 0.25))
-0.2698649654510865792581416
The dn-function is doubly periodic with periods and
:
>>> dn = ellipfun('dn')
>>> dn(2, 0.25)
0.8764740583123262286931578
>>> dn(2+2*ellipk(0.25), 0.25)
0.8764740583123262286931578
>>> chop(dn(2+4*j*ellipk(1-0.25), 0.25))
0.8764740583123262286931578
Evaluates the Klein j-invariant, which is a modular function defined for
in the upper half-plane as
where and
are the modular invariants of the Weierstrass
elliptic function,
An alternative, common notation is that of the j-function
.
Examples
Verifying the functional equation :
>>> from mpmath import *
>>> mp.dps = 25; mp.pretty = True
>>> tau = 0.625+0.75*j
>>> tau = 0.625+0.75*j
>>> kleinj(tau)
(-0.1507492166511182267125242 + 0.07595948379084571927228948j)
>>> kleinj(tau+1)
(-0.1507492166511182267125242 + 0.07595948379084571927228948j)
>>> kleinj(-1/tau)
(-0.1507492166511182267125242 + 0.07595948379084571927228946j)
The j-function has a famous Laurent series expansion in terms of the nome
,
:
>>> mp.dps = 15
>>> taylor(lambda q: 1728*q*kleinj(qbar=q), 0, 5, singular=True)
[1.0, 744.0, 196884.0, 21493760.0, 864299970.0, 20245856256.0]
The j-function admits exact evaluation at special algebraic points related to the Heegner numbers 1, 2, 3, 7, 11, 19, 43, 67, 163:
>>> @extraprec(10)
... def h(n):
... v = (1+sqrt(n)*j)
... if n > 2:
... v *= 0.5
... return v
...
>>> mp.dps = 25
>>> for n in [1,2,3,7,11,19,43,67,163]:
... n, chop(1728*kleinj(h(n)))
...
(1, 1728.0)
(2, 8000.0)
(3, 0.0)
(7, -3375.0)
(11, -32768.0)
(19, -884736.0)
(43, -884736000.0)
(67, -147197952000.0)
(163, -262537412640768000.0)
Also at other special points, the j-function assumes explicit algebraic values, e.g.:
>>> chop(1728*kleinj(j*sqrt(5)))
1264538.909475140509320227
>>> identify(cbrt(_)) # note: not simplified
'((100+sqrt(13520))/2)'
>>> (50+26*sqrt(5))**3
1264538.909475140509320227