Math Functions

There are a number of built-in math functions which take and return vectors. Generally, these functions operate on the supplied vector term-by-term, returning a vector of the same length as that given.

The pre-defined functions available are listed below. In general, all operations and functions will work on either real or complex values, providing complex data output when necessary.

In addition, there are statistical random number sources, and a number of compatibility functions to support HSPICE extensions available. These are described in sections that follow.

It should be noted that the mathematics subsystem used to evaluate expressions in voltage/current sources is completely different. In that subsystem, functions take real valued scalars as input. Although many of the same functions are available in both systems, the correspondence is not absolute.

`abs(`*vector*)

Each point of the returned vector is the absolute value of the corresponding point of*vector*. This is the same as the`mag`function.`acos(`*vector*)

Each point of the returned vector is the arc-cosine of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`acosh(`*vector*)

Each point of the returned vector is the arc-hyperbolic cosine of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`asin(`*vector*)

Each point of the returned vector is the arc-sine of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`asinh(`*vector*)

Each point of the returned vector is the arc-hyperbolic sine of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`atan(`*vector*)

Each point of the returned vector is the arc-tangent of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`atanh(`*vector*)

Each point of the returned vector is the arc-hyperbolic tangent of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`cbrt(`*vector*)

Each point of the returned vector is a cube root of the corresponding point of*vector*.`ceil(`*vector*)

This function returns the smallest integer greater than or equal to the argument, in the manner of the C function of the same name. If the argument is complex, the operation is performed on both components, with the result being complex. This operation is performed at each point in the given*vector*.`cos(`*vector*)

Each point of the returned vector is the cosine of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`cosh(`*vector*)

Each point of the returned vector is the hyperbolic cosine of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`db(`*vector*)

Each point of the returned vector is the decibel value (`20 * log10(mag)`) of the corresponding point of*vector*.`deriv(`*vector*)

This calculates the derivative of the given*vector*, using numeric differentiation by interpolating a polynomial. However, it may be prone to numerical errors, particularly with iterated differentiation. The implementation only calculates the derivative with respect to the real component of that vector's scale. The polynomial degree used for differentiation can be specified with the*dpolydegree*variable. If*dpolydegree*is unset, the value taken is 2 (quadratic). The valid range is 0-7.`erf(`*vector*)

Each point of the real returned vector is the error function of the corresponding real point of*vector*. Unlike most of the functions, this function operates only on the real part of a complex argument, and always returns a real valued result.`erfc(`*vector*)

Each point of the real returned vector is the complementary error function of the corresponding real point of*vector*. Unlike most of the functions, this function operates only on the real part of a complex argument, and always returns a real valued result.`exp(`*vector*)

Each point of the returned vector is the exponentiation (*e*^{x}) of the corresponding point of*vector*.`fft(`*vector*)

The`fft`function returns the Fourier transform of*vector*, using the present scale of*vector*. The scale should be linear and monotonic. The length is zero-padded to the next binary power. Only the real values are considered in the transform, so that the negative frequency terms are the complex conjugates of the positive frequency terms. The negative frequency terms are not included in the (complex) vector returned. A scale for the returned vector is also generated and linked to the returned vector.`floor(`*vector*)

This function returns the largest integer less than or equal to the argument, in the manner of the C function of the same name. If the argument is complex, the operation is performed on both components, with the result being complex. The operation is performed at each point of the argument.`gamma(`*vector*)

This function returns the gamma value of the real argument (or the real part of a complex argument), returning real data.`ifft(`*vector*)

The`ifft`function returns the inverse Fourier transform of*vector*, using the present scale of*vector*. The scale should be linear and monotonically increasing, starting at 0. Negative frequency terms are assumed to be complex conjugates of the positive frequency terms. The length is zero-padded to the next binary power. A scale for the returned vector is also generated and linked to the returned vector. The returned vector is always real.`im(`*vector*)

Each point of the real returned vector is the imaginary part of the corresponding point of the given*vector*. This function can also be calld as ```imag`''.`int(`*vector*)

The returned value is the nearest integer to the argument, in the manner of the C`rint`function. If the argument is complex, the operation is performed on each component with the result being complex. The operation is performed at each point in the argument.`integ(`*vector*)

The returned vector is the (trapezoidal) integral of*vector*with respect to the*vector*'s scale (which must exist).`interpolate(`*vector*)

This function takes its data and interpolates it onto a grid which is determined by the default scale of the currently active plot. The degree is determined by the*polydegree*variable. This is useful if the argument belongs to a plot which is not the current one. Some restrictions are that the current scale, the*vector*'s scale, and the argument must be real, and that either both scales must be strictly increasing or strictly decreasing if they differ.This function is used when operating on vectors from different plots, where the scale may differ. For example, the x-increment may be different, or the points may correspond to internal time points from transient analysis rather than the user time points. Without interpolation, operations are generally term-by-term, padding when necessary. This result is probably not useful if the scales are different.

For example, the correct way to print the difference between a vector in the current plot and a vector from another plot with a different scale would be

`print v(2) - interpolate(tran2.v(2))``j(`*vector*)

Each point of the returned vector is the corresponding point of*vector*multiplied by the square root of -1.`j0(`*vector*)

Each point of the real returned vector is the Bessel order 0 function of the corresponding real point of*vector*. Unlike most of the functions, this function operates only on the real part of a complex argument, and always returns a real valued result.`j1(`*vector*)

Each point of the real returned vector is the Bessel order 1 function of the corresponding real point of*vector*. Unlike most of the functions, this function operates only on the real part of a complex argument, and always returns a real valued result.`jn`(*n*,*vector*)

Each point of the real returned vector is the Bessel order*n*function of the corresponding real point of*vector*, with*n*the truncated integer value of the imaginary part of*vector*.Recall that for most math function, comma argument separators are interpreted as the comma operator

`a,b = (a + j*b)``jn(v,3)`'' where`v`is a real vector, the return will be`j3(v)`for each element of`v`.If

*vector*is real, the effective value of*n*is 0.`length(`*vector*)

This function returns the scalar length of*vector*.`ln(`*vector*)

Each point of the returned vector is the natural logarithm of the corresponding point of*vector*.`log(`*vector*)

Each point of the returned vector is the base-10 logarithm of the corresponding point of*vector*.`log10(`*vector*)

Each point of the returned vector is the natural logarithm of the corresponding point of*vector*(same as`ln`).**Warning:**in releases prior to 3.2.15, the`log`function returned the base-10 logarithm (as in Berkeley SPICE3). This was changed in 3.2.15 for compatibility with device simulation models intended for HSPICE.`mag(`*vector*)

Each point of the real returned vector is the magnitude of the corresponding point of*vector*.`mean(`*vector*)

This function returns the (scalar) mean value of the elements in the argument.`norm(`*vector*)

Each point of the returned vector is the corresponding point of the given vector multiplied by the magnitude of the inverse of the largest value in the given vector. The returned vector is therefor normalized to 1 (i. e, the largest magnitude of any component will be 1).`ph(`*vector*)

Each point of the real returned vector is the phase of the corresponding point of*vector*, expressed in radians.`pos(`*vector*)

This function returns a real vector which is 1 if the corresponding element of the argument has a non-zero real part, and 0 otherwise.`re(`*vector*)

Each point of the real returned vector is the real part of the corresponding point of*vector*. The function can also be called as ```real`''.`rms(`*vector*)

This function integrates the magnitude-squared of*vector*over the*vector*'s scale (using trapezoidal integration), divides by the scale range, and returns the square root of this result. If the*vector*has no scale, the square root of the sum of the squares of the elements is returned.`sgn(`*vector*)

Each value of the output vector is 1, 0, or -1 according to whether the corresponding value of the input vector is larger than 0, equal to zero, or less than 0. The vector can be complex or real.`sin(`*vector*)

Each point of the returned vector is the sine of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`sinh(`*vector*)

Each point of the returned vector is the hyperbolic sine of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`sqrt(`*vector*)

Each point of the returned vector is the square root of the corresponding point of*vector*.`sum(`*vector*)

This function returns the (scalar) sum of the elements of*vector*.`tan(`*vector*)

Each point of the returned vector is the tangent of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`tanh(`*vector*)

Each point of the returned vector is the hyperbolic tangent of the corresponding point of*vector*. This and all trig functions operate with radians unless the*units*variable is set to`degrees`.`unitvec(`*vector*)

This function returns a real vector consisting of all 1's, with length equal to the magnitude of the first element of the argument.`vector(`*vector*)

This function returns a vector consisting of the integers from 0 up to the magnitude of the first element of its argument.`y0(`*vector*)

Each point of the real returned vector is the Neumann order 0 function of the corresponding real point of*vector*. Unlike most of the functions, this function operates only on the real part of a complex argument, and always returns a real valued result.`y1(`*vector*)

Each point of the real returned vector is the Neumann order 1 function of the corresponding real point of*vector*. Unlike most of the functions, this function operates only on the real part of a complex argument, and always returns a real valued result.`yn`(*n*,*vector*)

Each point of the real returned vector is the Neumann order*n*function of the corresponding real point of*vector*, with*n*the truncated integer value of the imaginary part.Recall that for most math function, comma argument separators are interpreted as the comma operator

`a,b = (a + j*b)``yn(v,3)`'' where`v`is a real vector, the return will be`y3(v)`for each element of`v`.If

*vector*is real, the effective value of*n*is 0.