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research [2018/02/09 10:42]
rubiola [Cryogenic Sapphire Oscillators]
research [2018/03/05 14:03]
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-‹P^I—•QA¹k©¨}¦ë·ñ׏ªn£ö±­ƒÌ½žLñŸx¡3g×òZ‰óÒ[ë̋(šŽ8·m‹§®•Ϥ1âÔ©_[Ug‘<z/ƒ¶µ >ˆ¯š¼<lêÕ×wŽæ⷏'​“Wk]¯D°"​”J4åÆëLQËÐ:%lÁ¯ô¤¤ŠBeပó"​“umƒX*!½ð¸Íð/)VÖæâT.Ýfz®TöNÏ÷… +^[[Home]]^[[News]]^[[Stability&​Noise]]^[[Research]]^[[Services]]^[[Links]]^[[Venue]]^[[Contacts]]^ 
-ÒØúPˆSë`U{á”ô¶>kÅÇÉY\Ù: + 
-åFS§LpÍ0!n©HBµ@a@‚aŒ­}ªª`½¥äâØVË~"​fxØîb¢žb¤Ný°¨ér · Ÿ 6VWxv^qOGW‰ G¼3è¤sćº¶êù«š&​ÏÀH¹é:™e­“ñ&​`‡Éã6½‡1…ŽîÝYÜ¿?ßb:​8…‘+ɅtìuluÐQh‡"​²,õåE ²º²qØóìd6mZ¦y؍D#​Š8û ¥¶ã¬ /öžƒa”«kÍ'​÷©ôÇ ˆ!\©š +====== Microwave Photonics ====== 
-¡0 É šÖ0{Žl£‚æ¹C*ý´ÄûX“ÿüñûÑÝ9+ 
-#​2F„ÚY€Ÿŗ`« žª¸rxAдcUT™<​:m + 
-pYÀnsO§5jmyŠúށE?®‰Wº·Gý[ætžƒAj©-=r~ÇÜþÐ<​Së½Nۇ±ÙÛ8SÒ²”©Ý+§»náØ +== Pound Drever Hall Frequency Stabilization == 
-_‰B긣QüuœÚqrþOœihŒrIå»Å5%] + 
-M'x}ææìÞ ‹YÈ#​³5kéÝ +{{ :​pdh.png?​320 |}} 
-†ã±rŽhO_¨›mPoÙקÑÓË :a´þ¹fJð˜HÌ + 
-‹Ä +Owing to the physical nature of the lasing effect, lasers cannot be as stable as a good Fabry-Perot (FP) etalon. ​ For this reason, we stabilize our reference lasers to different types of Fabry-Perot etalons, depending on needs. ​ The Pound-Drever-Hall is the scheme that exhibits the highest reliability,​ and also the most suitable to ultimate frequency stability. ​  
-k"&​Â;​ë¨à«ª³ÐAÊñ÷³^§RŠ…1§~£íÐiŸ`áGIź¡ýôâg/​~f?ýu½Ü+öyÃÝ.é  ÄÆ#​O°S¯Tˆhôª’Ӵ餣y"​:ú̯°p#​‚Ç$׊¿/​ÒªãÂ<​]þҌ±q5Ímqºóva'​slÎ2lKÓGÏ1„èuLÙ Ù4¥FØ_ùL} •§ÿþacØ =ÀÁÏ¥³~ºVK¶yïË­­‘nê7Cˆ#​0ˆY¾^Mi ¹Mä“ 7v¾½Ìßz{‚t©±B_ðý#​ÿ“ðD¯°íñ!òßùÈ>​­ÂuÜËþ+ 
 +The laser is frequency modulated at a suitable frequency ​//f<sub>m</sub>// of the order of 20 MHz and several orders of magnitude higher than the FP cavity linewidth. ​ With the scheme shown, the cavity transforms the phase modulation into amplitude modulation, which is detected by a photodiode. ​ The control delivers a DC signal proportional to the frequency detuning of the laser vs the reference cavity. ​  
 + 
 + 
 +== Temperature Turning Point == 
 + 
 + 
 +{{ :ule-temperature.png?​320 |}} 
 + 
 +A temperature turning point is a key element in the design of a high-stability cavity because spacer and mirrors suffer from thermal expansion. ​ A thermal expansion //ΔL/L// causes a shift //​Δf/​f=-ΔL/​L=//​ in the laser frequency. ​ Thermal expansion also causes geometric warp, mor difficult to explain and model. ​  
 + 
 +For reference, the thermal expansion is of the order of 10<​sup>​-5</​sup>/​K for metals, and of the order of 10<​sup>​-6</​sup>/​K for glass and ceramics. ​ Thus, the unrealistic temperature stability of 0.1-1 nK would be necessary for a frequency stability of 10<​sup>​-15</​sup>​. 
 + 
 +A well designed cavity exhibits a smooth turning point. ​ If the cavity is stabilized at the turning point //​T<​sub>​0</​sub>//,​ the thermal expansion is proportional to (//​T-T<​sub>​0</​sub>/​/)<​sup>​2</​sup>​ As temperature stability of 10-100 μK is therefore sufficient ​ 
 +to stabilize the laser frequency at 10<sup>-15</​sup>​ level. 
 + 
 + 
 + 
 + 
 +== Femtosecond Comb == 
 + 
 +{{ :comb.png?​320 |}} 
 + 
 +The femtosecond comb is the standard tool to refer the optical frequency of laser to a reference frequency in the radio spectrum. ​ The comb enables to transfer the accuracy of the primary standard, the 9.192631770 GHz resonance of the Cs atom, to the optical signal. ​  
 +Such frequency transfer is so good that the fluctuations are of parts in 10<​sup>​-16</​sup>​ at 1 (Allan deviation) 
 + 
 +A femtosecond laser generates light pulses at a repetition rate //​f<​sub>​rep</​sub>​≈250//​ MHz.  These pulses are  so sharp that the harmonics span over more than one octave. ​ Beating two lines //​f<​sub>​1</​sub>//​ and //​f<​sub>​2</​sub>//​ spaced by one octave (//​f<​sub>​2</​sub>​≈2f<​sub>​1</​sub>//​),​ it is possible to lock the difference //​f<​sub>​2</​sub>​-f<​sub>​1</​sub>//​ to //​f<​sub>​1</​sub>//​. ​ In this condition, the repetition rate //​f<​sub>​rep</​sub>//​ is frequency locked to the optical frequency. ​  
 + 
 + 
 + 
 +== Flicker Noise == 
 + 
 +Flicker (//1/f//) frequency noise in the FP cavity is powered by thermal energy //​k<​sub>​B</​sub>​T 
 +according to the law 
 +{{ :sdeltal.png?120 |}} 
 +where //f/ is the Fourier frequencyand //Q// is the mechanical of the material. 
 +Converting the PSD //​S_<​sub>​δL</​sub>​(f)// into Allan deviation of the fractional frequency, we get 
 +{{ :sigma-cavity.png?​200 |}} 
 + 
 + 
 +=== Our FP Cavities === 
 + 
 + 
 +{{ :​sphere-1.jpg?200 |}} 
 + 
 + 
 +{{ :small-cavity.jpg?​200 |}} 
 + 
 + 
 + 
 +{{ :​si-cavity.jpg?​200 |}} 
 + 
 + 
 +{{ :​si-cryostat.jpg?​200 |}} 
 + 
 +====== Cryogenic Sapphire Oscillators =====
 + 
 + 
 + 
 +{{ :​elisa-cerebros-web.jpg?​640 |}
 + 
 + 
 +{{ :solar-system.png?​640 |}} 
 + 
 + 
 + 
 +{{ :​wg-mode.png?640 |}} 
 + 
 + 
 + 
 +{{ :​sapphire-temperature.png?640 |}} 
 + 
 + 
 + 
 +{{ :csos-web.jpg?​640 |}
 + 
 + 
 +====== Time System ====== 
 + 
 + 
 + 
 +====== Digital Electronics ====== 
 + 
 + 
 + 
 + 
 +====== Metrology ====== 
 + 
 + 
  • research.txt
  • Last modified: 2019/02/05 19:12
  • by rubiola