Sum frequency generation process for a new astronomical instrument

We propose an exotic use of sum frequency generation process (SFG) to develop a new kind of high resolution interferometer for astronomical imaging. SFG is well known to be intrinsically a noiseless non linear process of upconversion which permits a wavelength shift. Thereby we propose to shift astronomical MIR and FIR radiation to shorter wavelength where optical fibers and optical components are available and efficient. In order to demonstrate the validity of this method for high resolution imaging, we plan to set up a two-arm upconversion interferometer on the CHARA telescope array (California). Each arm would include an upconversion stage at the focus of telescope. The success of such a project is obviously conditioned by the quality of nonlinear components (waveguided PPLN) in term of efficiency and noise biases. Moreover, coherence study requires the use of identical non linear components which implies manufacturing constraints. To ensure the feasibility of this project, several studies have been conducted. By implementing an upconversion interferometer in laboratory we have recently demonstrated our ability to analyze the coherence properties of a 1550nm signal at visible wavelength. We also have successfully converted astronomical light using one arm of this interferometer at the Hawaï observatory. It showed the capability of our instrument to astronomical observing conditions in photon counting regime. A preliminary mission at CHARA observatory allowed us to check the compatibility of our instrument with the environment onsite and expected photometric levels. From these data we estimate to be able to study the coherence of astronomical target at 1550nm using such an instrument.

[1]  N. Ye,et al.  Nonlinear optical crystal BiAlGa2(BO3)4 , 2007 .

[2]  Jean-Emmanuel Broquin,et al.  MAFL experiment: development of photonic devices for a space-based multiaperture fiber-linked interferometer. , 2007, Applied optics.

[3]  A. Yariv,et al.  Quantum Fluctuations and Noise in Parametric Processes. I. , 1961 .

[4]  A Tonello,et al.  Laboratory demonstration of an infrared-to-visible up-conversion interferometer for spatial coherence analysis. , 2008, Physical review letters.

[5]  Laurent Delage,et al.  Contrast and phase closure acquisitions in photon counting regime using a frequency upconversion interferometer for high angular resolution imaging , 2013 .

[6]  Laurent Delage,et al.  Analysis and control of polarization effects on phase closure and image acquisition in a fibre-linked three-telescope stellar interferometer , 2000 .

[7]  H. Herrmann,et al.  Application of frequency conversion of starlight to high-resolution imaging interferometry. On-sky sensitivity test of a single arm of the interferometer , 2012 .

[8]  H. Takesue,et al.  Efficient and low-noise single-photon detection in 1550 nm communication band by frequency upconversion in periodically poled LiNbO3 waveguides. , 2008, Optics letters.

[9]  F. Reynaud,et al.  Linear optical path modulation with lambda /200 accuracy using a fibre stretcher , 1993 .

[10]  H. Herrmann,et al.  Demonstration of a frequency spectral compression effect through an up-conversion interferometer. , 2013, Optics express.

[11]  Phase closure retrieval in an infrared-to-visible upconversion interferometer for high resolution astronomical imaging. , 2011, Optics express.

[12]  Lijun Ma,et al.  Tunable up-conversion detector for single photon and bi-photon infrared spectroscopic applications , 2013, Defense, Security, and Sensing.

[13]  R. Boyd Infrared Upconversion for Astronomy , 1977 .

[14]  High‐quantum‐efficiency infrared up‐conversion , 1973 .

[15]  M. Fejer,et al.  Ultralow noise up-conversion detector and spectrometer for the telecom band. , 2013, Optics express.

[16]  N. Gisin,et al.  Tunable upconversion photon detector , 2008, 0807.3399.

[17]  Stephen T. Ridgway,et al.  FLUOR fibered beam combiner at the CHARA array , 2003, SPIE Astronomical Telescopes + Instrumentation.