2019
DOI: 10.1364/oe.27.034192
|View full text |Cite
|
Sign up to set email alerts
|

81 supra-THz beams generated by a Fourier grating and a quantum cascade laser

Abstract: J-R. (2019). 81 supra-THz beams generated by a Fourier grating and a quantum cascade laser. Optics Express, 27(23), 34193-34204. https://doi.Abstract: Large heterodyne receiver arrays (~100 pixel) allow astronomical instrumentations to map more area within limited space mission lifetime. One challenge is to generate multiple local oscillator (LO) beams. Here, we succeeded in generating 81 beams at 3.86 THz by combining a reflective, metallic Fourier grating with an unidirectional antenna coupled 3rdorder distr… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
9
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
5
3

Relationship

4
4

Authors

Journals

citations
Cited by 15 publications
(9 citation statements)
references
References 30 publications
0
9
0
Order By: Relevance
“…The [OI] array for GUSTO includes 2×4 superconducting hot-electron bolometer (HEB) receivers. The required performance metrics for the local oscillator at 4.7 THz were calculated by researchers at SRON and the University of Arizona to ensure the proper performance of HEB receiver array and phase grating integrated with the optical set-up and explained in detail in [13][14][15]. By taking into account the optical loss due to the non-Gaussian beam pattern of THz QCLs, phase grating, and the available cooling power, the overall performance metrics were calculated and listed in table I.…”
Section: A Required Performance Metrics For Lo At 47 Thzmentioning
confidence: 99%
“…The [OI] array for GUSTO includes 2×4 superconducting hot-electron bolometer (HEB) receivers. The required performance metrics for the local oscillator at 4.7 THz were calculated by researchers at SRON and the University of Arizona to ensure the proper performance of HEB receiver array and phase grating integrated with the optical set-up and explained in detail in [13][14][15]. By taking into account the optical loss due to the non-Gaussian beam pattern of THz QCLs, phase grating, and the available cooling power, the overall performance metrics were calculated and listed in table I.…”
Section: A Required Performance Metrics For Lo At 47 Thzmentioning
confidence: 99%
“…Thus, the efficiency of the spatial filter is enhanced. One can use a lens and an iris aperture to achieve a quasi-Gaussian beam, as our group did in [21], but the efficiency is very low (∼10%). Two off-axis parabolic mirrors combined with a pinhole can also be used as a beam filter with an efficiency of 22% [22], but the system is bulky and the alignment of the whole system is challenging.…”
Section: Back-to-back Lens Systemmentioning
confidence: 99%
“…for the Galactic/Extragalactic ULDB Spectroscopic Terahertz Observatory (GUSTO) and the Stratospheric Observatory for Infrared Astronomy (SOFIA) [18,19]. For heterodyne mixer arrays, phase gratings are used as the multiplexer, which diffracts a single QCL beam into multiple beams as an array LO [20] and recently reported up to 81 beams [21]. To avoid overlap between the individual diffracted beams, a Gaussian input beam to the grating is required [22,23].…”
mentioning
confidence: 99%
“…Although it has a certain beam shaping effect, the transmissivity of the filtering system is only 22%. One can use a lens and an iris aperture to achieve a quasi-Gaussian beam [4], but the efficiency is very low (~10%). Another terahertz spatial filter is a back-to-back corrugated horn structure, whose principle is to eliminate the high-order Gaussian modes and random fluctuations of a source at microwave frequencies by using the mode conversion characteristic of corrugated horn and antenna reciprocity theorem [5].…”
Section: Introductionmentioning
confidence: 99%