Echelle Grating E230M

Description

The E230M grating is used with the NUV-MAMA and provides echelle spectra at a resolving power of 30,000 from 1607 to 3129 Å.

Special Considerations

A single exposure with this grating covers 800 Å over ~20–40 orders. The interorder separation is ~18 pixels (0.52 arcseconds) at 1650 Å and 62.5 pixels (~1.8 arcseconds) at 3100 Å. The grating must be scanned, with exposures taken at two distinct settings to cover the full spectral range of the grating.


Grating

Spectral Range

Average
Dispersion
(Å/Pixel)

Dispersion,
Cross Dispersion
Plate Scales
(arcsec/pixel)

Tilts

Central
Wavelengths

Complete

Per Tilt

E230M

1607–3129

∼800

λ/60,000

0.035,0.029

Prime

1978, 2707


 

 

 

 

 

Secondary

2124, 2269, 2415, 2561

Figure 13.46: Wavelength Ranges for the E230M Grating Setting.


E230M Sensitivities


Table 13.13: E230M Sensitivities & Throughputs for a Point Source.

λ

Sensitivity

% Throughput

1700

1.2E11

0.1

1800

2.5E11

0.2

1900

3.7E11

0.2

2000

5.1E11

0.3

2100

7.6E11

0.4

2200

1.0E12

0.6

2300

1.3E12

0.7

2400

1.4E12

0.7

2500

1.6E12

0.7

2600

1.7E12

0.7

2700

1.7E12

0.7

2800

1.7E12

0.7

2900

1.4E12

0.5

3000

1.1E12

0.4

3100

4.5E11

0.2

Figure 13.47: E230M Point Source (left axis), and Diffuse Source (right axis) Sensitivities.

Throughput curve traces the peaks of the blaze function for each order.

Note:

Point source sensitivity assumes full transmission (zero slit losses). Diffuse source sensitivity assumes a 0.1" wide slit. To convert point source sensitivities to diffuse source sensitivities multiply the point source values by the grating spatial (cross dispersion) plate scale in units of arcseconds per pixel and by the width of the desired slit in units of arcseconds.

E230M Signal-to-Noise

Note:

The top axis displays constant Fλ values corresponding to the STMAG units (V+STMAGλ) on the bottom axis. Recall that STMAG=0 is equivalent to Fλ = 3.63E–9 erg/cm2/s/Å. The curves are labeled with exposure times in seconds.

Figure 13.48: Diffuse Source Signal-to-Noise as a Function of STMAG for E230M.


Figure 13.49: Point Source Signal-to-Noise as a Function of STMAG for E230M.