A sensitive pressure sensor for diamond anvil cell experiments up to 2 GPa: FluoSpheres ®

We present an optical pressure sensor suitable for experiments in diamond anvil cell in the 0.1 MPa–2 GPa pressure range, for temperatures between ambient and 323 K. It is based on the pressure-dependent fluorescence spectrum of FluoSpheres®, which are commercially available fluorescent microspheres commonly used to measure blood flow in experimental biology. The fluorescence of microspheres is excited by the 514.5 nm line of an Ar+ laser, and the resulting spectrum displays three very intense broad bands at 534, 558, and 598 nm, respectively. The reference wavelength and pressure gauge is that of the first inflection point of the spectrum, located at 525.6±0.2 nm at ambient pressure. It is characterized by an instantaneous and large linear pressure shift of 9.93(±0.08) nm/GPa. The fluorescence of the FluoSpheres® has been investigated as a function of pressure (0.1–4 GPa), temperature (295–343 K), pH (3–12), salinity, and pressure transmitting medium. These measurements show that, for pressures comprised between 0.1 MPa and 2 GPa, at temperatures not exceeding 323 K, at any pH, in aqueous pressure transmitting media, pressure can be calculated from the wavelength shift of two to three beads, according to the relation P=0.100 (±0.001) Deltalambdai(P) with Deltalambdai(P)=lambdai(P)–lambdai(0) and lambdai(P) as the wavelength of the first inflection point of the spectrum at the pressure P. This pressure sensor is approximately thirty times more sensitive than the ruby scale and responds instantaneously to pressure variations.

[1]  P. Oger,et al.  Development of a low-pressure diamond anvil cell and analytical tools to monitor microbial activities in situ under controlled P and T. , 2006, Biochimica et biophysica acta.

[2]  A. Polian,et al.  Quartz as a pressure sensor in the infrared , 2005 .

[3]  J. Chervin,et al.  Pressure vessels for in vivo studies of deep-sea fauna , 2004 .

[4]  P. Loubeyre,et al.  Properties of diamond under hydrostatic pressures up to 140 GPa , 2003, Nature materials.

[5]  B. Reynard,et al.  Optimization of Sm3+ fluorescence in Sm-doped yttrium aluminum garnet: Application to pressure calibration in diamond-anvil cell at high temperature , 2002 .

[6]  M. Mancinelli,et al.  Erratum: “ruby-spheres as pressure gauge for optically transparent high pressure cells” , 2001 .

[7]  O. Grasset Calibration of the R ruby fluorescence lines in the pressure range [0-1 GPa] and the temperature range [250-300 K] , 2001 .

[8]  J. Sturgis,et al.  The effect of pressure on the bacteriochlorophyll a binding sites of the core antenna complex from Rhodospirillum rubrum. , 1998, Biochemistry.

[9]  P. Loubeyre,et al.  Improved calibration of the SrB4O7:Sm2+ optical pressure gauge: Advantages at very high pressures and high temperatures , 1997 .

[10]  J. Leger,et al.  SrB4O7 : Sm2+ pressure optical sensor : investigations in the megabar range , 1990 .

[11]  N. Hess,et al.  Pressure and temperature dependence of laser‐induced fluorescence of Sm:YAG to 100 kbar and 700 °C and an empirical model , 1990 .

[12]  G. Exarhos,et al.  Temperature and pressure dependence of laser induced fluorescence in Sm:YAG—a new pressure calibrant , 1989 .

[13]  C. Chateau,et al.  High‐pressure measurements at moderate temperatures in a diamond anvil cell with a new optical sensor: SrB4O7:Sm2+ , 1989 .

[14]  J. W. Shaner,et al.  Specific volume measurements of Cu, Mo, Pd, and Ag and calibration of the ruby R1 fluorescence pressure gauge from 0.06 to 1 Mbar , 1978 .

[15]  H. Mao,et al.  High-Pressure Physics: The 1-Megabar Mark on the Ruby R1 Static Pressure Scale , 1976, Science.

[16]  S. Block,et al.  Pressure Measurement Made by the Utilization of Ruby Sharp-Line Luminescence , 1972, Science.

[17]  M. Eremets High Pressure Experimental Methods , 1996 .

[18]  Stanley Block,et al.  An Optical Fluorescence System for Quantitative Pressure Measurement in the Diamond‐Anvil Cell , 1973 .