Typical XUV pulse intensity required to produce nonlinear processes is of the order of 1012-1014 W/cm2 [1], which can be achieved by increasing the energy of the XUV pulses and/or by decreasing the corresponding spot size in the target region. Additional requirements are the following: (i) use of a setup characterized by a sufficiently long exit arm, while maintaining a compact size, in order to accommodate different experimental devices in the target region; (ii) generation of two XUV pulse replica, with adjustable temporal delay (accuracy of the order of 10 as).

High-throughput and microfocusing capabilities of a beamline for attosecond pulses based on toroidal mirrors

F Frassetto;M Nisoli;L Poletto
2015

Abstract

Typical XUV pulse intensity required to produce nonlinear processes is of the order of 1012-1014 W/cm2 [1], which can be achieved by increasing the energy of the XUV pulses and/or by decreasing the corresponding spot size in the target region. Additional requirements are the following: (i) use of a setup characterized by a sufficiently long exit arm, while maintaining a compact size, in order to accommodate different experimental devices in the target region; (ii) generation of two XUV pulse replica, with adjustable temporal delay (accuracy of the order of 10 as).
2015
ultrafast
microfocusing
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/355092
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