Characterization of collisionally pumped optical-field-ionization soft X-ray lasers
We give an overview of recent experimental results on optical-field-ionization collisional soft X-ray lasers developed at LOA. By focusing a 30-fs, circularly polarized Ti-sapphire laser pulse at an intensity of up to 8X10 Wcm into a low-density gas cell containing Xe or Kr, we produced a few mm lon...
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| Veröffentlicht in: | Applied physics. B, Lasers and optics Lasers and optics, 2004-05, Vol.78 (7-8), p.939-944 |
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| container_title | Applied physics. B, Lasers and optics |
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| creator | MOCEK, T SEBBAN, S CARILLON, A JAMELOT, G RUS, B WYART, J. F BETTAIBI, I UPCRAFT, L. M BALCOU, P BREGER, P ZEITOUN, P LE PAPE, S ROS, D KLISNICK, A |
| description | We give an overview of recent experimental results on optical-field-ionization collisional soft X-ray lasers developed at LOA. By focusing a 30-fs, circularly polarized Ti-sapphire laser pulse at an intensity of up to 8X10 Wcm into a low-density gas cell containing Xe or Kr, we produced a few mm long plasma column for soft X-ray amplifier. Saturated amplification has been achieved on the 4d5d(S0)--4d5p(P1) transition at 41.8 nm in Xe, and on the 3d4d(S0)--3d4p(P1) transition in Kr at 32.8 nm. Under optimum pumping conditions the Xe laser provides about (5c2)X10 photons per pulse whilst the Kr laser delivers up to (2.5c1)X10 photons per shot. The repetition rate of these soft X-ray lasers is 10 Hz. The beam wavefront of the Xe laser has been measured by a Shack--Hartmann soft X-ray wavefront sensor, and the pulse duration by a cross-correlation technique. |
| doi_str_mv | 10.1007/s00340-004-1436-3 |
| format | Article |
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The repetition rate of these soft X-ray lasers is 10 Hz. The beam wavefront of the Xe laser has been measured by a Shack--Hartmann soft X-ray wavefront sensor, and the pulse duration by a cross-correlation technique.</description><identifier>ISSN: 0946-2171</identifier><identifier>EISSN: 1432-0649</identifier><identifier>DOI: 10.1007/s00340-004-1436-3</identifier><language>eng</language><publisher>Berlin: Springer</publisher><subject>Beams (radiation) ; Exact sciences and technology ; Focusing ; Fundamental areas of phenomenology (including applications) ; Laser-plasma interactions ; Lasers ; Optics ; Optimization ; Photons ; Physics ; Physics of gases, plasmas and electric discharges ; Physics of plasmas and electric discharges ; Plasma production and heating ; Plasma production and heating by laser beams ; Shot ; Soft x-rays ; Wave fronts ; Wavefronts ; X- and γ-ray lasers</subject><ispartof>Applied physics. 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Saturated amplification has been achieved on the 4d5d(S0)--4d5p(P1) transition at 41.8 nm in Xe, and on the 3d4d(S0)--3d4p(P1) transition in Kr at 32.8 nm. Under optimum pumping conditions the Xe laser provides about (5c2)X10 photons per pulse whilst the Kr laser delivers up to (2.5c1)X10 photons per shot. The repetition rate of these soft X-ray lasers is 10 Hz. The beam wavefront of the Xe laser has been measured by a Shack--Hartmann soft X-ray wavefront sensor, and the pulse duration by a cross-correlation technique.</description><subject>Beams (radiation)</subject><subject>Exact sciences and technology</subject><subject>Focusing</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Laser-plasma interactions</subject><subject>Lasers</subject><subject>Optics</subject><subject>Optimization</subject><subject>Photons</subject><subject>Physics</subject><subject>Physics of gases, plasmas and electric discharges</subject><subject>Physics of plasmas and electric discharges</subject><subject>Plasma production and heating</subject><subject>Plasma production and heating by laser beams</subject><subject>Shot</subject><subject>Soft x-rays</subject><subject>Wave fronts</subject><subject>Wavefronts</subject><subject>X- and γ-ray lasers</subject><issn>0946-2171</issn><issn>1432-0649</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><recordid>eNqFkU1rGzEQhkVoIW7aH5DbXgrpQcnoYyXtMZjmAww5pIXexFgrEQXZ2krrgvvrK-MkPWYuGknP-zLMS8g5g0sGoK8qgJBAASRlUigqTsiiNZyCksMHsoBBKsqZZqfkU63P0EoZsyCPyycs6GZf4l-cY952OXQupxRru2BK-27abSY_dnmao8NEQ_RppO3zVVBzmLtftOC-S1h9qZ_Jx4Cp-i8v5xn5efP9x_KOrh5u75fXK-qEFjP1PIzKjagQNDMyrEXgyqHzwLgSatDrQfK1E8prY_Ra6hGc0YpDCK6HXokz8u3o-4TJTiVusOxtxmjvrlf28AbQc66Z_sMae3Fkp5J_73yd7SZW51PCrc-7apnSbV2618P7KDdCGc2BN5QdUVdyrcWHtzEY2EMu9phLm0TaQy5WNM3XF3usbZ-h4NbF-l_YawnMCPEPm9aMlA</recordid><startdate>20040501</startdate><enddate>20040501</enddate><creator>MOCEK, T</creator><creator>SEBBAN, S</creator><creator>CARILLON, A</creator><creator>JAMELOT, G</creator><creator>RUS, B</creator><creator>WYART, J. 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B, Lasers and optics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>MOCEK, T</au><au>SEBBAN, S</au><au>CARILLON, A</au><au>JAMELOT, G</au><au>RUS, B</au><au>WYART, J. F</au><au>BETTAIBI, I</au><au>UPCRAFT, L. M</au><au>BALCOU, P</au><au>BREGER, P</au><au>ZEITOUN, P</au><au>LE PAPE, S</au><au>ROS, D</au><au>KLISNICK, A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Characterization of collisionally pumped optical-field-ionization soft X-ray lasers</atitle><jtitle>Applied physics. B, Lasers and optics</jtitle><date>2004-05-01</date><risdate>2004</risdate><volume>78</volume><issue>7-8</issue><spage>939</spage><epage>944</epage><pages>939-944</pages><issn>0946-2171</issn><eissn>1432-0649</eissn><abstract>We give an overview of recent experimental results on optical-field-ionization collisional soft X-ray lasers developed at LOA. By focusing a 30-fs, circularly polarized Ti-sapphire laser pulse at an intensity of up to 8X10 Wcm into a low-density gas cell containing Xe or Kr, we produced a few mm long plasma column for soft X-ray amplifier. Saturated amplification has been achieved on the 4d5d(S0)--4d5p(P1) transition at 41.8 nm in Xe, and on the 3d4d(S0)--3d4p(P1) transition in Kr at 32.8 nm. Under optimum pumping conditions the Xe laser provides about (5c2)X10 photons per pulse whilst the Kr laser delivers up to (2.5c1)X10 photons per shot. The repetition rate of these soft X-ray lasers is 10 Hz. The beam wavefront of the Xe laser has been measured by a Shack--Hartmann soft X-ray wavefront sensor, and the pulse duration by a cross-correlation technique.</abstract><cop>Berlin</cop><pub>Springer</pub><doi>10.1007/s00340-004-1436-3</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0002-5546-6436</orcidid></addata></record> |
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| subjects | Beams (radiation) Exact sciences and technology Focusing Fundamental areas of phenomenology (including applications) Laser-plasma interactions Lasers Optics Optimization Photons Physics Physics of gases, plasmas and electric discharges Physics of plasmas and electric discharges Plasma production and heating Plasma production and heating by laser beams Shot Soft x-rays Wave fronts Wavefronts X- and γ-ray lasers |
| title | Characterization of collisionally pumped optical-field-ionization soft X-ray lasers |
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