SpecDisperser.py

from astropy.table import Table

import astropy.constants as cons

import collections
from collections import OrderedDict
from scipy import interpolate

from astropy import units as u

# from numpy import *

import numpy as np

from pylab import *

import galsim

import sys
import os
import math


def rotate90(array_orig=None, xc=0, yc=0, isClockwise=0):
    if array_orig is None:
        return

    l1 = array_orig.shape[0]
    l2 = array_orig.shape[1]

    if xc < 0 or xc > l2 - 1 or yc < 0 or yc > l1 - 1:
        return

    n_xc = xc
    n_yc = yc

    array_final = np.zeros_like(array_orig.T)

    if isClockwise == 1:
        for i in np.arange(l2):
            array_final[i] = array_orig[:, l2 - i - 1]
        n_xc = yc
        n_yc = l2 - 1 - xc
    else:
        for i in np.arange(l2):
            array_final[i] = array_orig[::-1, i]

        n_xc = l1 - 1 - yc
        n_yc = xc
    return array_final, n_xc, n_yc


class SpecDisperser(object):
    def __init__(
        self,
        orig_img=None,
        xcenter=0,
        ycenter=0,
        origin=[100, 100],
        tar_spec=None,
        band_start=6200,
        band_end=10000,
        isAlongY=0,
        conf="../param/CONF/csst.conf",
        gid=0,
        flat_cube=None,
        ignoreBeam=[],
    ):
        """
        orig_img: normal image,galsim image
        xcenter, ycenter: the center of galaxy in orig_img
        origin : [int, int]
            `origin` defines the lower left pixel index (y,x) of the `direct`
            cutout from a larger detector-frame image
        tar_spec: galsim.SED

        """

        # self.img_x = orig_img.shape[1]
        # self.img_y = orig_img.shape[0]

        # 5 orders, A, B ,
        orderName = ["A", "B", "C", "D", "E"]
        self.orig_img_orders = OrderedDict()
        if isinstance(orig_img, list):
            orig_img_list = orig_img
            list_len = len(orig_img_list)
            if list_len < 5:
                for i in np.arange(5 - list_len):
                    orig_img_list.append(orig_img_list[list_len - 1])
            for i, k in enumerate(orig_img_list):
                self.orig_img_orders[orderName[i]] = k

        if isinstance(orig_img, galsim.Image):
            for i in np.arange(5):
                self.orig_img_orders[orderName[i]] = orig_img

        orig_img_one = self.orig_img_orders["A"]

        self.thumb_img = np.abs(orig_img_one.array)
        self.thumb_x = orig_img_one.center.x
        self.thumb_y = orig_img_one.center.y
        self.img_sh = orig_img_one.array.shape

        self.id = gid

        self.xcenter = xcenter
        self.ycenter = ycenter

        self.isAlongY = isAlongY
        self.flat_cube = flat_cube
        if self.isAlongY == 1:
            for order in orderName:
                self.orig_img_orders[order], self.thumb_x, self.thumb_y = rotate90(
                    array_orig=self.orig_img_orders[order],
                    xc=orig_img_one.center.x,
                    yc=orig_img_one.center.y,
                    isClockwise=1,
                )
            # self.thumb_img, self.thumb_x, self.thumb_y = rotate90(array_orig=self.thumb_img, xc=orig_img_one.center.x,
            #                                                       yc=orig_img_one.center.y, isClockwise=1)

            self.img_sh = self.orig_img_orders[order].array.T.shape
            self.xcenter = ycenter
            self.ycenter = xcenter

        self.origin = origin
        self.band_start = band_start
        self.band_end = band_end
        self.spec = tar_spec

        self.beam_flux = OrderedDict()

        self.grating_conf = aXeConf(conf)
        self.grating_conf.get_beams()
        self.grating_conf_file = conf
        self.ignoreBeam = ignoreBeam

    def compute_spec_orders(self):

        all_orders = OrderedDict()
        beam_names = self.grating_conf.beams

        for beam in beam_names:
            if beam in self.ignoreBeam:
                continue
            all_orders[beam] = self.compute_spec(beam)

        return all_orders

    def compute_spec(self, beam):

        # if beam == "B":
        #     return self.thumb_img, self.origin[1], self.origin[0], None, None, None

        from .disperse_c import interp
        from .disperse_c import disperse

        # from MockObject.disperse_c import disperse
        self.thumb_img = np.abs(self.orig_img_orders[beam].array)
        self.thumb_x = self.orig_img_orders[beam].center.x
        self.thumb_y = self.orig_img_orders[beam].center.y
        self.img_sh = self.orig_img_orders[beam].array.shape
        dx = self.grating_conf.dxlam[beam]
        xoff = 0
        ytrace_beam, lam_beam = self.grating_conf.get_beam_trace(
            x=self.xcenter, y=self.ycenter, dx=(dx + xoff), beam=beam
        )

        # Account for pixel centering of the trace
        yfrac_beam = ytrace_beam - floor(ytrace_beam + 0.5)

        ysens = lam_beam * 0
        lam_index = argsort(lam_beam)
        conf_sens = self.grating_conf.sens[beam]

        lam_intep = np.linspace(self.band_start, self.band_end, int(
            (self.band_end - self.band_start) / 0.1))

        thri = interpolate.interp1d(
            conf_sens["WAVELENGTH"], conf_sens["SENSITIVITY"])
        spci = interpolate.interp1d(self.spec["WAVELENGTH"], self.spec["FLUX"])

        beam_thr = thri(lam_intep)
        spec_sample = spci(lam_intep)

        bean_thr_spec = beam_thr * spec_sample

        # generate sensitivity file for aXe
        # ysensitivity = lam_beam * 0
        #
        # ysensitivity[lam_index] = interp.interp_conserve_c(lam_beam[lam_index], lam_intep,
        #                                                    beam_thr * math.pi * 100 * 100 * 1e-7 / (
        #                                                                cons.h.value * cons.c.value / (
        #                                                                    lam_intep * 1e-10)), integrate=0, left=0,
        #                                                    right=0)
        #
        # self.writerSensitivityFile(conffile = self.grating_conf_file,  beam = beam, w = lam_beam[lam_index], sens = ysensitivity[lam_index])

        ysens[lam_index] = interp.interp_conserve_c(
            lam_beam[lam_index], lam_intep, bean_thr_spec, integrate=1, left=0, right=0
        )

        sensitivity_beam = ysens

        len_spec_x = len(dx)
        len_spec_y = int(
            abs(ceil(ytrace_beam[-1]) - floor(ytrace_beam[0])) + 1)

        beam_sh = (self.img_sh[0] + len_spec_y, self.img_sh[1] + len_spec_x)
        modelf = zeros(product(beam_sh), dtype=float)
        model = modelf.reshape(beam_sh)
        idx = np.arange(modelf.size, dtype=int64).reshape(beam_sh)
        x0 = array((self.thumb_y, self.thumb_x), dtype=int64)

        dxpix = dx - dx[0] + x0[1]

        dyc = cast[int](np.floor(ytrace_beam + 0.5))

        # dypix = cast[int](np.floor(ytrace_beam - dyc[0] + x0[0] + 0.5))
        dypix = dyc - dyc[0] + x0[0]

        frac_ids = yfrac_beam < 0

        dypix[frac_ids] = dypix[frac_ids] - 1
        yfrac_beam[frac_ids] = 1 + yfrac_beam[frac_ids]

        flat_index = idx[dypix, dxpix]

        nonz = sensitivity_beam != 0

        origin_in = zeros_like(self.origin)
        dx0_in = dx[0]
        dy0_in = dyc[0]
        if self.isAlongY == 1:
            origin_in[0] = self.origin[0]
            origin_in[1] = self.origin[1] - len_spec_y
            dx0_in = -dyc[0]
            dy0_in = dx[0]
        else:
            origin_in[0] = self.origin[0]
            origin_in[1] = self.origin[1]
            dx0_in = dx[0]
            dy0_in = dyc[0]
            originOut_x = origin_in[1] + dx0_in
        originOut_y = origin_in[0] + dy0_in

        if self.flat_cube is None:
            beam_flat = None
        else:
            beam_flat = zeros([len(modelf), len(self.flat_cube)])

            sub_flat_cube = zeros(
                [len(self.flat_cube), beam_sh[0], beam_sh[1]])
            sub_flat_cube[0] = sub_flat_cube[0] + 1.0

            overlap_flag = 1

            sub_y_s = originOut_y
            sub_y_e = originOut_y + beam_sh[0] - 1
            sub_x_s = originOut_x
            sub_x_e = originOut_x + beam_sh[1] - 1

            beam_x_s = max(sub_x_s, 0)
            if beam_x_s > self.flat_cube[0].shape[1] - 1:
                overlap_flag = 0
            if overlap_flag == 1:
                beam_x_e = min(sub_x_e, self.flat_cube[0].shape[1] - 1)
                if beam_x_e < 0:
                    overlap_flag = 0

            if overlap_flag == 1:
                beam_y_s = max(sub_y_s, 0)
                if beam_y_s > self.flat_cube[0].shape[0] - 1:
                    overlap_flag = 0
            if overlap_flag == 1:
                beam_y_e = min(sub_y_e, self.flat_cube[0].shape[0] - 1)
                if beam_y_e < 0:
                    overlap_flag = 0

            if overlap_flag == 1:
                sub_flat_cube[
                    :,
                    beam_y_s - originOut_y: beam_y_e - originOut_y + 1,
                    beam_x_s - originOut_x: beam_x_e - originOut_x + 1,
                ] = self.flat_cube[:, beam_y_s: beam_y_e + 1, beam_x_s: beam_x_e + 1]

            for i in arange(0, len(self.flat_cube), 1):
                beam_flat[:, i] = sub_flat_cube[i].flatten()
        #            beam_flat = zeros([len(modelf), len(self.flat_cube)])
        #            flat_sh = self.flat_cube[0].shape
        #            for i in arange(0, beam_sh[0], 1):
        #                for j in arange(0, beam_sh[1], 1):
        #                    k = i * beam_sh[1] + j
        #                    if originOut_y + i >= flat_sh[0] or originOut_y + i < 0 or originOut_x + j>= flat_sh[1] or originOut_x+j < 0:
        #                        temp_bf = np.zeros_like(self.flat_cube[:, 0, 0])
        #                        temp_bf[0] = 1.0
        #                        beam_flat[k] = temp_bf
        #                    else:
        #                        beam_flat[k] = self.flat_cube[:, originOut_y + i, originOut_x + j]

        status = disperse.disperse_grism_object(
            self.thumb_img.astype(np.float32),
            flat_index[nonz],
            yfrac_beam[nonz],
            sensitivity_beam[nonz],
            modelf,
            x0,
            array(self.img_sh, dtype=int64),
            array(beam_sh, dtype=int64),
            beam_flat,
            lam_beam[lam_index][nonz],
        )

        model = modelf.reshape(beam_sh)
        # n1 = np.sum(np.isinf(model))
        # n2 = np.sum(np.isnan(model))
        # n3 = np.sum(np.isinf(modelf))
        # n4 = np.sum(np.isnan(modelf))
        # if n1>0 or n2 > 0:
        #     print("DEBUG: SpecDisperser, inf:%d, nan:%d--------%d,%d"%(n1, n2, n3, n4))
        #     print(dypix)
        # n1 = np.sum(np.isinf(self.thumb_img.astype(np.float32)))
        # n2 = np.sum(np.isnan(self.thumb_img.astype(np.float32)))
        # n3 = np.sum(np.isinf(yfrac_beam))
        # n4 = np.sum(np.isnan(yfrac_beam))
        # n5 = np.sum(np.isinf(sensitivity_beam))
        # n6 = np.sum(np.isnan(sensitivity_beam))
        # print("DEBUG: SpecDisperser, innput ---inf:%d, nan:%d, yfrac_beam:%d/%d, sensitivity_beam:%d/%d"%(n1, n2, n3, n4, n5, n6))
        self.beam_flux[beam] = sum(modelf)

        if self.isAlongY == 1:
            model, _, _ = rotate90(array_orig=model, isClockwise=0)
        return model, originOut_x, originOut_y, dxpix, dypix, lam_beam, ysens

    def writerSensitivityFile(self, conffile="", beam="", w=None, sens=None):
        orders = {"A": "1st", "B": "0st", "C": "2st", "D": "-1st", "E": "-2st"}
        sens_file_name = conffile[0:-5] + \
            "_sensitivity_" + orders[beam] + ".fits"
        if os.path.exists(sens_file_name) is False:
            senstivity_out = Table(
                array([w, sens]).T, names=("WAVELENGTH", "SENSITIVITY"))
            senstivity_out.write(sens_file_name, format="fits")


"""
Demonstrate aXe trace polynomials.
"""


class aXeConf:
    def __init__(self, conf_file="WFC3.IR.G141.V2.5.conf"):
        """Read an aXe-compatible configuration file

        Parameters
        ----------
        conf_file: str
            Filename of the configuration file to read

        """
        if conf_file is not None:
            self.conf = self.read_conf_file(conf_file)
            self.conf_file = conf_file
            self.count_beam_orders()

            # Global XOFF/YOFF offsets
            if "XOFF" in self.conf.keys():
                self.xoff = np.float(self.conf["XOFF"])
            else:
                self.xoff = 0.0

            if "YOFF" in self.conf.keys():
                self.yoff = np.float(self.conf["YOFF"])
            else:
                self.yoff = 0.0

    def read_conf_file(self, conf_file="WFC3.IR.G141.V2.5.conf"):
        """Read an aXe config file, convert floats and arrays

        Parameters
        ----------
        conf_file: str
            Filename of the configuration file to read.

        Parameters are stored in an OrderedDict in `self.conf`.
        """
        from collections import OrderedDict

        conf = OrderedDict()
        lines = open(conf_file).readlines()
        for line in lines:
            # empty / commented lines
            if (line.startswith("#")) | (line.strip() == "") | ('"' in line):
                continue

            # split the line, taking out ; and # comments
            spl = line.split(";")[0].split("#")[0].split()
            param = spl[0]
            if len(spl) > 2:
                value = np.cast[float](spl[1:])
            else:
                try:
                    value = float(spl[1])
                except:
                    value = spl[1]

            conf[param] = value

        return conf

    def count_beam_orders(self):
        """Get the maximum polynomial order in DYDX or DLDP for each beam"""
        self.orders = {}
        for beam in ["A", "B", "C", "D", "E", "F", "G", "H", "I", "J"]:
            order = 0
            while "DYDX_{0:s}_{1:d}".format(beam, order) in self.conf.keys():
                order += 1

            while "DLDP_{0:s}_{1:d}".format(beam, order) in self.conf.keys():
                order += 1

            self.orders[beam] = order - 1

    def get_beams(self):
        """Get beam parameters and read sensitivity curves"""
        import os
        from collections import OrderedDict
        from astropy.table import Table, Column

        self.dxlam = OrderedDict()
        self.nx = OrderedDict()
        self.sens = OrderedDict()
        self.beams = []

        for beam in self.orders:
            if self.orders[beam] > 0:
                self.beams.append(beam)
                self.dxlam[beam] = np.arange(
                    self.conf["BEAM{0}".format(beam)].min(), self.conf["BEAM{0}".format(beam)].max(), dtype=int
                )
                self.nx[beam] = int(self.dxlam[beam].max() -
                                    self.dxlam[beam].min()) + 1
                self.sens[beam] = Table.read(
                    "{0}/{1}".format(os.path.dirname(self.conf_file),
                                     self.conf["SENSITIVITY_{0}".format(beam)])
                )
                # self.sens[beam].wave = np.cast[np.double](self.sens[beam]['WAVELENGTH'])
                # self.sens[beam].sens = np.cast[np.double](self.sens[beam]['SENSITIVITY'])

                # Need doubles for interpolating functions
                for col in self.sens[beam].colnames:
                    data = np.cast[np.double](self.sens[beam][col])
                    self.sens[beam].remove_column(col)
                    self.sens[beam].add_column(Column(data=data, name=col))

        self.beams.sort()

    def field_dependent(self, xi, yi, coeffs):
        """aXe field-dependent coefficients

        See the `aXe manual <http://axe.stsci.edu/axe/manual/html/node7.html#SECTION00721200000000000000>`_ for a description of how the field-dependent coefficients are specified.

        Parameters
        ----------
        xi, yi : float or array-like
            Coordinate to evaluate the field dependent coefficients, where
            `xi = x-REFX` and `yi = y-REFY`.

        coeffs : array-like
            Field-dependency coefficients

        Returns
        -------
        a : float or array-like
            Evaluated field-dependent coefficients

        """
        # number of coefficients for a given polynomial order
        # 1:1, 2:3, 3:6, 4:10, order:order*(order+1)/2
        if isinstance(coeffs, float):
            order = 1
        else:
            order = int(-1 + np.sqrt(1 + 8 * len(coeffs))) // 2

        # Build polynomial terms array
        # $a = a_0+a_1x_i+a_2y_i+a_3x_i^2+a_4x_iy_i+a_5yi^2+$ ...
        xy = []
        for p in range(order):
            for px in range(p + 1):
                # print 'x**%d y**%d' %(p-px, px)
                xy.append(xi ** (p - px) * yi ** (px))

        # Evaluate the polynomial, allowing for N-dimensional inputs
        a = np.sum((np.array(xy).T * coeffs).T, axis=0)

        return a

    def evaluate_dp(self, dx, dydx):
        # """Evalate arc length along the trace given trace polynomial coefficients

        # Parameters
        # ----------
        # dx : array-like
        #     x pixel to evaluate

        # dydx : array-like
        #     Coefficients of the trace polynomial

        # Returns
        # -------
        # dp : array-like
        #     Arc length along the trace at position `dx`.

        # For `dydx` polynomial orders 0, 1 or 2, integrate analytically.
        # Higher orders must be integrated numerically.

        # **Constant:**
        #     .. math:: dp = dx

        # **Linear:**
        #     .. math:: dp = \sqrt{1+\mathrm{DYDX}[1]}\cdot dx

        # **Quadratic:**
        #     .. math:: u = \mathrm{DYDX}[1] + 2\ \mathrm{DYDX}[2]\cdot dx

        #     .. math:: dp = (u \sqrt{1+u^2} + \mathrm{arcsinh}\ u) / (4\cdot \mathrm{DYDX}[2])

        # """
        # dp is the arc length along the trace
        # $\lambda = dldp_0 + dldp_1 dp + dldp_2 dp^2$ ...

        poly_order = len(dydx) - 1
        if poly_order == 2:
            if np.abs(np.unique(dydx[2])).max() == 0:
                poly_order = 1

        if poly_order == 0:  # dy=0
            dp = dx
        elif poly_order == 1:  # constant dy/dx
            dp = np.sqrt(1 + dydx[1] ** 2) * (dx)
        elif poly_order == 2:  # quadratic trace
            u0 = dydx[1] + 2 * dydx[2] * (0)
            dp0 = (u0 * np.sqrt(1 + u0**2) + np.arcsinh(u0)) / (4 * dydx[2])
            u = dydx[1] + 2 * dydx[2] * (dx)
            dp = (u * np.sqrt(1 + u**2) + np.arcsinh(u)) / (4 * dydx[2]) - dp0
        else:
            # high order shape, numerical integration along trace
            # (this can be slow)
            xmin = np.minimum((dx).min(), 0)
            xmax = np.maximum((dx).max(), 0)
            xfull = np.arange(xmin, xmax)
            dyfull = 0
            for i in range(1, poly_order):
                dyfull += i * dydx[i] * (xfull - 0.5) ** (i - 1)

            # Integrate from 0 to dx / -dx
            dpfull = xfull * 0.0
            lt0 = xfull < 0
            if lt0.sum() > 1:
                dpfull[lt0] = np.cumsum(
                    np.sqrt(1 + dyfull[lt0][::-1] ** 2))[::-1]
                dpfull[lt0] *= -1

            #
            gt0 = xfull > 0
            if gt0.sum() > 0:
                dpfull[gt0] = np.cumsum(np.sqrt(1 + dyfull[gt0] ** 2))

            dp = np.interp(dx, xfull, dpfull)
            if dp[-1] == dp[-2]:
                dp[-1] = dp[-2] + np.diff(dp)[-2]

        return dp

    def get_beam_trace(self, x=507, y=507, dx=0.0, beam="A"):
        """Get an aXe beam trace for an input reference pixel and list of output x pixels `dx`

        Parameters
        ----------
        x, y : float or array-like
            Evaluate trace definition at detector coordinates `x` and `y`.

        dx : float or array-like
            Offset in x pixels from `(x,y)` where to compute trace offset and
            effective wavelength

        beam : str
            Beam name (i.e., spectral order) to compute.  By aXe convention,
            `beam='A'` is the first order, 'B' is the zeroth order and
            additional beams are the higher positive and negative orders.

        Returns
        -------
        dy : float or array-like
            Center of the trace in y pixels offset from `(x,y)` evaluated at
            `dx`.

        lam : float or array-like
            Effective wavelength along the trace evaluated at `dx`.

        """
        NORDER = self.orders[beam] + 1

        xi, yi = x - self.xoff, y - self.yoff
        xoff_beam = self.field_dependent(
            xi, yi, self.conf["XOFF_{0}".format(beam)])
        yoff_beam = self.field_dependent(
            xi, yi, self.conf["YOFF_{0}".format(beam)])

        # y offset of trace (DYDX)
        dydx = np.zeros(NORDER)  # 0 #+1.e-80
        dydx = [0] * NORDER

        for i in range(NORDER):
            if "DYDX_{0:s}_{1:d}".format(beam, i) in self.conf.keys():
                coeffs = self.conf["DYDX_{0:s}_{1:d}".format(beam, i)]
                dydx[i] = self.field_dependent(xi, yi, coeffs)

        # $dy = dydx_0+dydx_1 dx+dydx_2 dx^2+$ ...

        dy = yoff_beam
        for i in range(NORDER):
            dy += dydx[i] * (dx - xoff_beam) ** i

        # wavelength solution
        dldp = np.zeros(NORDER)
        dldp = [0] * NORDER

        for i in range(NORDER):
            if "DLDP_{0:s}_{1:d}".format(beam, i) in self.conf.keys():
                coeffs = self.conf["DLDP_{0:s}_{1:d}".format(beam, i)]
                dldp[i] = self.field_dependent(xi, yi, coeffs)

        self.eval_input = {"x": x, "y": y, "beam": beam, "dx": dx}
        self.eval_output = {
            "xi": xi,
            "yi": yi,
            "dldp": dldp,
            "dydx": dydx,
            "xoff_beam": xoff_beam,
            "yoff_beam": yoff_beam,
            "dy": dy,
        }

        dp = self.evaluate_dp(dx - xoff_beam, dydx)
        # ## dp is the arc length along the trace
        # ## $\lambda = dldp_0 + dldp_1 dp + dldp_2 dp^2$ ...
        # if self.conf['DYDX_ORDER_%s' %(beam)] == 0:   ## dy=0
        #     dp = dx-xoff_beam
        # elif self.conf['DYDX_ORDER_%s' %(beam)] == 1: ## constant dy/dx
        #     dp = np.sqrt(1+dydx[1]**2)*(dx-xoff_beam)
        # elif self.conf['DYDX_ORDER_%s' %(beam)] == 2: ## quadratic trace
        #     u0 = dydx[1]+2*dydx[2]*(0)
        #     dp0 = (u0*np.sqrt(1+u0**2)+np.arcsinh(u0))/(4*dydx[2])
        #     u = dydx[1]+2*dydx[2]*(dx-xoff_beam)
        #     dp = (u*np.sqrt(1+u**2)+np.arcsinh(u))/(4*dydx[2])-dp0
        # else:
        #     ## high order shape, numerical integration along trace
        #     ## (this can be slow)
        #     xmin = np.minimum((dx-xoff_beam).min(), 0)
        #     xmax = np.maximum((dx-xoff_beam).max(), 0)
        #     xfull = np.arange(xmin, xmax)
        #     dyfull = 0
        #     for i in range(1, NORDER):
        #         dyfull += i*dydx[i]*(xfull-0.5)**(i-1)
        #
        #     ## Integrate from 0 to dx / -dx
        #     dpfull = xfull*0.
        #     lt0 = xfull <= 0
        #     if lt0.sum() > 1:
        #         dpfull[lt0] = np.cumsum(np.sqrt(1+dyfull[lt0][::-1]**2))[::-1]
        #         dpfull[lt0] *= -1
        #     #
        #     gt0 = xfull >= 0
        #     if gt0.sum() > 0:
        #         dpfull[gt0] = np.cumsum(np.sqrt(1+dyfull[gt0]**2))
        #
        #     dp = np.interp(dx-xoff_beam, xfull, dpfull)

        # Evaluate dldp
        lam = dp * 0.0
        for i in range(NORDER):
            lam += dldp[i] * dp**i

        return dy, lam

    def show_beams(self, beams=["E", "D", "C", "B", "A"]):
        """
        Make a demo plot of the beams of a given configuration file
        """
        import matplotlib.pyplot as plt

        x0, x1 = 507, 507
        dx = np.arange(-800, 1200)

        if "WFC3.UV" in self.conf_file:
            x0, x1 = 2073, 250
            dx = np.arange(-1200, 1200)
        if "G800L" in self.conf_file:
            x0, x1 = 2124, 1024
            dx = np.arange(-1200, 1200)

        s = 200  # marker size
        fig = plt.figure(figsize=[10, 3])
        plt.scatter(0, 0, marker="s", s=s, color="black",
                    edgecolor="0.8", label="Direct")

        for beam in beams:
            if "XOFF_{0}".format(beam) not in self.conf.keys():
                continue

            xoff = self.field_dependent(
                x0, x1, self.conf["XOFF_{0}".format(beam)])
            dy, lam = self.get_beam_trace(x0, x1, dx=dx, beam=beam)
            xlim = self.conf["BEAM{0}".format(beam)]
            ok = (dx >= xlim[0]) & (dx <= xlim[1])
            plt.scatter(dx[ok] + xoff, dy[ok], c=lam[ok] / 1.0e4,
                        marker="s", s=s, alpha=0.5, edgecolor="None")
            plt.text(np.median(dx[ok]), np.median(
                dy[ok]) + 1, beam, ha="center", va="center", fontsize=14)
            print("Beam {0}, lambda=({1:.1f} - {2:.1f})".format(beam,
                  lam[ok].min(), lam[ok].max()))

        plt.grid()
        plt.xlabel(r"$\Delta x$")
        plt.ylabel(r"$\Delta y$")

        cb = plt.colorbar(pad=0.01, fraction=0.05)
        cb.set_label(r"$\lambda\,(\mu\mathrm{m})$")
        plt.title(self.conf_file)
        plt.tight_layout()
        plt.savefig("{0}.pdf".format(self.conf_file))

    # def load_grism_config(conf_file):


#     """Load parameters from an aXe configuration file

#     Parameters
#     ----------
#     conf_file : str
#         Filename of the configuration file

#     Returns
#     -------
#     conf : `~grizli.grismconf.aXeConf`
#         Configuration file object.  Runs `conf.get_beams()` to read the
#         sensitivity curves.
#     """
#     conf = aXeConf(conf_file)
#     conf.get_beams()
#     return conf