the stratospheric terahertz observatory...the stratospheric terahertz observatory johns hopkins apl...

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H.  K.  CHARLES  ET AL. JOHNS HOPKINS APL TECHNICAL DIGEST,  VOLUME 28, NUMBER 3 (2010) 238 collaborative effort led by the University of Arizona and APL with a significant contribution from the JHU Department of Physics and Astronomy. STO is a balloon-borne observing platform that will carry an 80-cm-aperture telescope in the stratosphere at an altitude of ~120,000 ft. The telescope will feed a het- erodyne receiver consisting of eight phonon-cooled hot- electron bolometer (HEB) mixers, four optimized for the dominant interstellar cooling line [CII] (at 158 μm) and four for the important star-formation tracer [NII] line (at 205 μm). The spectrometer has a resolving power, R, of >1,000,000 and an angular resolution of 1 arcmin, which is sufficient to spatially resolve atomic, ionic, and molec- ular clouds at 10 kpc. It will have sufficient bandwidth to detect all clouds participating in galactic rotation in each of the 8 pixels. STO is capable of detecting every giant molecular cloud in our galaxy, every HII region of sig- nificance, and every diffuse HI cloud with visual extinc- Figure 1. (a) Sample ISM map and the corresponding spectrum. (b) Map of Antarctica with the projected path of the STO flight. (c) Region of our galaxy surveyed by STO. The Stratospheric Terahertz Observatory P. N. Bernasconi*, D. Neufeld , C. Walker , D. Hollenbach § , J. Kawamura , and J. Stuzki || *JHU Applied Physics Laboratory, Laurel, MD; JHU Department of Physics and Astronomy, Baltimore, MD; University of Arizona, Tuscon, AZ; § SETI Institute, Mountain View, CA; Jet Propulsion Laboratory, Pasadena, CA; and | | University of Köln, Köln, Germany 50 100 –5 0 5 10 Every “pixel” represents a high-resolution spectrum! 100 0 1 0 1 0 T (K) HI Galactic longitude (degrees) 10 –5 erg/s/cm 2 /sr V LSR (km/s) (C II) 300 s (C II) 15 s CO J = 1-0 HI 21 cm Balloon trajectory McMurdo station Ross Ice Shelf –10 T (K) CO 4 2 0 George V Land (a) (b) (c) T he Stratospheric Terahertz Observatory (STO) is a long-duration balloon (LDB) experiment designed to address a key problem in modern astrophysics: namely, understanding the life cycle of the galactic interstellar medium (ISM). STO is a

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Page 1: The Stratospheric Terahertz Observatory...THE STRATOSPHERIC TERAHERTZ OBSERVATORY JOHNS HOPKINS APL TECHNICAL DIGEST, VOLUME 28, NUMBER 3 (2010) 239 tion greater than 0.3 magnitudes

H.  K.  CHARLES  et al.

JOHNS HOPKINS APL TECHNICAL DIGEST,  VOLUME 28, NUMBER 3 (2010)238

collaborative effort led by the University of Arizona and APL with a significant contribution from the JHU Department of Physics and Astronomy.

STO is a balloon-borne observing platform that will carry an 80-cm-aperture telescope in the stratosphere at an altitude of ~120,000 ft. The telescope will feed a het-erodyne receiver consisting of eight phonon-cooled hot-electron bolometer (HEB) mixers, four optimized for the dominant interstellar cooling line [CII] (at 158 μm) and

four for the important star-formation tracer [NII] line (at 205 μm). The spectrometer has a resolving power, R, of >1,000,000 and an angular resolution of 1 arcmin, which is sufficient to spatially resolve atomic, ionic, and molec-ular clouds at 10 kpc. It will have sufficient bandwidth to detect all clouds participating in galactic rotation in each of the 8 pixels. STO is capable of detecting every giant molecular cloud in our galaxy, every HII region of sig-nificance, and every diffuse HI cloud with visual extinc-

Figure 1. (a) Sample ISM map and the corresponding spectrum. (b) Map of Antarctica with the projected path of the STO flight. (c) Region of our galaxy surveyed by STO.

The Stratospheric Terahertz Observatory

P. N. Bernasconi*, D. Neufeld†, C. Walker‡, D. Hollenbach§, J. Kawamura¶, and J. Stuzki||

*JHU Applied Physics Laboratory, Laurel, MD; †JHU Department of Physics and Astronomy, Baltimore, MD; ‡University of Arizona, Tuscon, AZ; §SETI Institute,

Mountain View, CA; ¶Jet Propulsion Laboratory, Pasadena, CA; and ||University of Köln, Köln, Germany

50 100

–50510

Every “pixel” represents a high-resolution spectrum!

100

0

1

0

1

0

T (

K)

HI

Galactic longitude (degrees)

10–5

erg

/s/c

m2 /s

r

VLSR (km/s)

(C II) 300 s

(C II) 15 s

CO J = 1-0HI 21 cm

Balloontrajectory

McMurdostation

Ross Ice Shelf

T (

K)

CO

–10

T (

K)

CO4

2

0

George V Land

(a) (b) (c)

The Stratospheric Terahertz Observatory (STO) is a long-duration balloon (LDB) experiment designed to address a key problem in modern astrophysics: namely,

understanding the life cycle of the galactic interstellar medium (ISM). STO is a

Page 2: The Stratospheric Terahertz Observatory...THE STRATOSPHERIC TERAHERTZ OBSERVATORY JOHNS HOPKINS APL TECHNICAL DIGEST, VOLUME 28, NUMBER 3 (2010) 239 tion greater than 0.3 magnitudes

THE STRATOSPHERIC TERAHERTZ OBSERVATORY

JOHNS HOPKINS APL TECHNICAL DIGEST,  VOLUME 28, NUMBER 3 (2010) 239­­­­

tion greater than 0.3 magnitudes (Fig. 1a).

STO had a 1-day test flight in mid-October 2009 from Fort Sumner, NM. In December 2010, it will have its first LDB flight of approximately 15 days from Ant-arctica (Fig. 1b).

During the Antarctic flight, it will survey a section of the galactic plane in both CII and NII (Fig. 1c). Combined with previous HI and CO surveys, STO will create 3-D maps of the structure, dynamics, turbulence, energy balance, and pressure of the Milky Way’s ISM, as well as the star-formation rate. Our mission goals for this survey are to (i) determine the life cycle of galactic interstellar gas, (ii) study the creation and disruption of star-forming clouds in our galaxy, (iii) determine the parameters that affect the star-formation rate in the galaxy, and (iv) provide tem-plates for star formation and stel-lar/ interstellar feedback in other galaxies.

For the STO program, APL will provide the telescope, the observ-ing platform (gondola), the point-ing system, the power system, the

For further information on the work reported here, see the references below or contact [email protected].

1Bernasconi, P. N., Rust, D. M., Eaton, H. A. C., and Murphy, G. A., “A Balloon-Borne Telescope for High-Resolution Solar Imaging and Polarimetry,” in Airborne Telescopes Systems, R. K. Melugin and H.-P. Röser (eds.), Proc. of SPIE, Vol. 4014, SPIE, Bellingham, WA, pp. 214–225, doi: 10.1117/12.389100 (2000).

2Bernasconi, P. N., Eaton, H. A. C., Foukal, P., and Rust, D. M., “The Solar Bolometric Imager,” Adv. Space Res. 33, 1746 (2004).

Figure 2. (a) STO telescope assembled and installed on gondola. (b) Diagram of STO tele-scope optical path and attached test flight relay optics box and Dewar. (c) Dummy Dewar installed on back of telescope. (d) Cutaway of FIR spectrometer for STO test flight.

command and control system, and the ground support equipment to interface with NASA telemetry system (Fig. 2). The University of Arizona will design, build, and operate the spectrometer. The JHU Department

of Physics and Astronomy will provide guidance in determining the observing plan and contribute with the reduction and analysis of the data from the STO flights.

Primarymirror

Internalbaffles

Relay optics boxDewar

Optical path

HEB mixers(detectors)

DewarControl

electronicsbox

(b)

(d)

(a)(a)

(c)

Secondarymirror