Integration
- galsim.integ.int1d(func, min, max, rel_err=1e-06, abs_err=1e-12)[source]
- Integrate a 1-dimensional function from min to max. - Example usage: - >>> def func(x): return x**2 >>> galsim.integ.int1d(func, 0, 1) 0.33333333333333337 >>> galsim.integ.int1d(func, 0, 2) 2.666666666666667 >>> galsim.integ.int1d(func, -1, 1) 0.66666666666666674 - Note - This uses an adaptive Gauss-Kronrod-Patterson method for doing the integration. - cf. https://www.jstor.org/stable/2004583 - If one or both endpoints are infinite, it will automatically use an appropriate transformation to turn it into a finite integral. - Parameters:
- func – The function to be integrated. y = func(x) should be valid. 
- min – The lower end of the integration bounds (anything < -1.e10 is treated as negative infinity). 
- max – The upper end of the integration bounds (anything > 1.e10 is treated as positive infinity). 
- rel_err – The desired relative error [default: 1.e-6] 
- abs_err – The desired absolute error [default: 1.e-12] 
 
- Returns:
- the value of the integral. 
 
- galsim.integ.hankel(func, k, nu=0, rmax=None, rel_err=1e-06, abs_err=1e-12)[source]
- Perform an order nu Hankel transform of the given function f(r) at a specific k value. \[F(k) = \int_0^\infty f(r) J_\nu(k r) r dr\]- Note - For non-truncated Hankel integrals, this uses the method outlined in Ogata, 2005: http://www.kurims.kyoto-u.ac.jp/~prims/pdf/41-4/41-4-40.pdf - For truncated integrals (and k=0), it uses the same adaptive Gauss-Kronrod-Patterson method used for - int1d.- Parameters:
- func – The function f(r) 
- k – (float or numpy array) The value(s) of k for which to calculate F(k). 
- nu – The order of the Bessel function to use for the transform. [default: 0] 
- rmax – An optional truncation radius at which to have f(r) drop to 0. [default: None] 
- rel_err – The desired relative accuracy [default: 1.e-6] 
- abs_err – The desired absolute accuracy [default: 1.e-12] 
 
- Returns:
- An estimate of F(k) 
 
- class galsim.integ.IntegrationRule[source]
- A class that can be used to integrate something more complicated than a normal scalar function. - In GalSim, we use it to do the integration of chromatic images over a bandpass. Typically f is some kind of draw function, xs are the wavelengths, and w is the bandpass throughput. But this class is abstracted away from all of that and can be used for anything where the function returns something complicated, but which can be added together to compute the quadrature. - Specifically the return value from f must be closed under both addition and multiplication by a scalar (a float value). 
- class galsim.integ.QuadRule[source]
- Quadratic rule for integration - This models both f and w as linear between the evaluation points, so the product is quadratic. 
- class galsim.integ.ImageIntegrator[source]
- A base class for integrators used by - ChromaticObjectto integrate the drawn images over wavelengthh using a- Bandpassas a weight function.- __call__(evaluateAtWavelength, bandpass, image, drawImageKwargs, doK=False)[source]
- Parameters:
- evaluateAtWavelength – Function that returns a monochromatic surface brightness profile as a function of wavelength. 
- bandpass – - Bandpassobject representing the filter being imaged through.
- image – - Imageused to set size and scale of output
- drawImageKwargs – dict with other kwargs to send to - ChromaticObject.drawImagefunction.
- doK – Integrate up results of - ChromaticObject.drawKImageinstead of results of- ChromaticObject.drawImage. [default: False]
 
- Returns:
- the result of integral as an - Image
 
 
- class galsim.integ.SampleIntegrator(rule)[source]
- Bases: - ImageIntegrator- Create a chromatic surface brightness profile integrator, which will integrate over wavelength using a - Bandpassas a weight function.- This integrator will evaluate the integrand only at the wavelengths in - bandpass.wave_list. See ContinuousIntegrator for an integrator that evaluates the integrand at a given number of points equally spaced apart.- Parameters:
- rule – - Which integration rule to apply to the wavelength and monochromatic surface brightness samples. Options include: - galsim.integ.midptRule: Use the midpoint integration rule 
- galsim.integ.trapzRule: Use the trapezoidal integration rule 
- galsim.integ.quadRule: Use the quadratic integration rule 
 
 
- class galsim.integ.ContinuousIntegrator(rule, N=250, use_endpoints=True)[source]
- Bases: - ImageIntegrator- Create a chromatic surface brightness profile integrator, which will integrate over wavelength using a - Bandpassas a weight function.- This integrator will evaluate the integrand at a given number - Nof equally spaced wavelengths over the interval defined by bandpass.blue_limit and bandpass.red_limit. See SampleIntegrator for an integrator that only evaluates the integrand at the predefined set of wavelengths in- bandpass.wave_list.- Parameters:
- rule – - Which integration rule to apply to the wavelength and monochromatic surface brightness samples. Options include: - galsim.integ.midptRule: Use the midpoint integration rule 
- galsim.integ.trapzRule: Use the trapezoidal integration rule 
- galsim.integ.quadRule: Use the quadratic integration rule 
 
- N – Number of equally-wavelength-spaced monochromatic surface brightness samples to evaluate. [default: 250] 
- use_endpoints – Whether to sample the endpoints - bandpass.blue_limitand- bandpass.red_limit. This should probably be True for a rule like numpy.trapz, which explicitly samples the integration limits. For a rule like the midpoint rule, however, the integration limits are not generally sampled, (only the midpoint between each integration limit and its nearest interior point is sampled), thus- use_endpointsshould be set to False in this case. [default: True]