Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. (a) Schematic of the noncollinear optical parametric amplification (NOPA) geometry.

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Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. (a) Schematic of the noncollinear optical parametric amplification (NOPA) geometry showing the geometry for pump, signal, and idler beam. (b) Laboratory picture of an optical parametric amplifier (OPA) setup with the green pump beam visible aligned through a BBO crystal. 37 Figure Legend: From: Concepts, performance review, and prospects of table-top, few-cycle optical parametric chirped-pulse amplification Opt. Eng. 2013;53(5): doi: /1.OE

Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. (a) Calculated parametric gain in dependence of the interaction length and the pump intensity. (b) Scaled 44 damage threshold 45,46 of BBO in the femtosecond to nanosecond range. Figure Legend: From: Concepts, performance review, and prospects of table-top, few-cycle optical parametric chirped-pulse amplification Opt. Eng. 2013;53(5): doi: /1.OE

Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. Traditional optical parametric chirped pulse amplification (OPCPA) architecture in the visible based upon a sub-5-fs oscillator, a pulse stretcher, the broadband amplification in the OPA, and a compressor to retrieve almost the original pulse duration. The pump beam is typically derived from the front-end oscillator to ensure optical synchronization and utilizes in the pump beam generation multiple amplification stages resulting in a high-energetic picosecond pump pulse. Figure Legend: From: Concepts, performance review, and prospects of table-top, few-cycle optical parametric chirped-pulse amplification Opt. Eng. 2013;53(5): doi: /1.OE

Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. The colored bars represent the few-cycle OPCPA bandwidth of reported systems for few different crystals, pump wavelengths, and phase matching condition. The gray bars represent the typical transparency range of the employed crystals. Note that the tuning range of the mentioned OPA stages can be larger than the indicated OPCPA bandwidths and extremely wide OPA tuning ranges covering the visible 55 to near-IR 65 and mid-IR 66 have been reported. Figure Legend: From: Concepts, performance review, and prospects of table-top, few-cycle optical parametric chirped-pulse amplification Opt. Eng. 2013;53(5): doi: /1.OE

Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. Graphical overview of the performance of reported OPCPA systems. A color code is employed to emphasize the impact of the pump laser technology on the overall OPCPA performance. See Table 1 for the list of references and Table 2 for the list of acronyms. Figure Legend: From: Concepts, performance review, and prospects of table-top, few-cycle optical parametric chirped-pulse amplification Opt. Eng. 2013;53(5): doi: /1.OE

Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. Performance of OPCPA pump lasers in terms of pulse energy and average power against the year of publication. The pump laser systems are differentiated by color code corresponding to their laser technology. See Table 3 for the list of references and Table 2 for the list of acronyms. Figure Legend: From: Concepts, performance review, and prospects of table-top, few-cycle optical parametric chirped-pulse amplification Opt. Eng. 2013;53(5): doi: /1.OE

Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. (a) Performances of the pump lasers of reported OPCPA systems in terms of pulse energy and average power. (b) Performance of recently demonstrated high-energy, high-average-power picosecond laser system. The laser systems are differentiated by color code corresponding to their laser technology. See Tables 3 and 4 for the list of references and Table 2 for the list of acronyms. Figure Legend: From: Concepts, performance review, and prospects of table-top, few-cycle optical parametric chirped-pulse amplification Opt. Eng. 2013;53(5): doi: /1.OE