Echelle Grating E140H

Description

The E140H grating is used with the NUV-MAMA and provides echelle spectra at a resolving power of ~114,0001 from ~1140 to 1700 Å.

Special Considerations

A single E140H echellogram covers ~210 Å, over ~50 orders. The order separation is ~16 pixels (0.47 arcseconds) at 1150 Å and ~36 pixels (1.05 arcseconds) at 1700 Å. The grating must be scanned, with exposures taken at three distinct settings to cover the full spectral range of the grating.

Note that while the spectral format of the 1234 Å setting extends down to 1133 Å, the throughput becomes vanishingly small below about 1140 Å.


Grating

Spectral Range

Average
Dispersion
(Å per Pixel)

Dispersion, Cross Dispersion Plate Scale
(arcsec/pixel)

Tilts

Central
Wavelengths

Complete

Per Tilt

E140H

1140–1700

∼210

λ/228,000

0.047,0.029

Prime

1234, 1416, 1598


 

 

 

 

 

Secondary

1271, 1307, 1343,
1380, 1453, 1489,
1526, 1562

Figure 13.58: Wavelength Ranges for the E140H Grating Setting.


E140H Sensitivities


Table 13.16: E140H Sensitivities & Throughputs for a Point Source.

λ

Sensitivity

% Throughput

1200

5.0E10

0.4

1250

9.4E10

0.6

1300

1.1E11

0.7

1350

1.0E11

0.6

1400

8.9E10

0.5

1450

7.3E10

0.4

1500

5.7E10

0.3

1550

4.2E10

0.2

1600

2.9E10

0.1

1650

2.2E10

0.1

Figure 13.59: E140H 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.

E140H 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 13.60: Diffuse Source Signal-to-Noise as a Function of STMAG for E14030H.


Figure 13.61: Point Source Signal-to-Noise as a Function of STMAG for E140H.




1 R ~ 200,000 possible with the 0.1X0.03 aperture; see Section 12.6.