绝热变频器作为自定义的跨倍频散元件

Dylan Heberle, Noah Flemens, Connor Davis, J. Moses
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摘要

色散管理是设计和实现具有八度跨度带宽和良好压缩脉冲质量的放大激光系统最具挑战性的方面之一。在这里,我们展示了一种新型的八度跨度色散管理装置。我们将啁啾准相位匹配(QPM)在频率转换过程中的脉冲整形范式与绝热频率下变频装置的鲁棒、高效、跨倍频的能力相结合。结果是一个简单的单片器件,可以产生具有定制色散的八度跨越红外脉冲-这种技术可能特别方便用于采用差频产生和/或参数放大级的高能放大器链。该技术还可以作为一种方法,在可见光到中红外光谱中产生持续时间约10秒的脉冲,用于高光谱超快光谱。绝热频率转换在啁啾QPM器件中采用缓慢变化的位置相关极点频率,以线性传递函数在宽带宽上有效地移频光子。在这项工作中,我们证明了该过程的频率相关局部转换允许裁剪总群延迟色散(GDD)。我们已经展示了一个零GDD的器件,允许将几个周期的近红外输入有效地转换为相同持续时间(~12 fs,带宽跨越2.0-4.0微米)的近单周期中红外输出。我们提出了精确定制频率相关群延迟的附加设计。
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Adiabatic frequency converter as a custom octave-spanning dispersive element
Dispersion management is among the most challenging aspects of the design and realization of amplified laser systems possessing octave-spanning bandwidth and good compressed pulse quality. Here we demonstrate a new type of device for octave-spanning dispersion management. We combine the paradigm of chirped quasi-phase matching (QPM) for pulse shaping during frequency conversion with the robust, efficient, octave-spanning capability of an adiabatic frequency downconversion device. The result is a simple, monolithic device that can produce an octave-spanning infrared pulse with tailored dispersion – a technique that may be especially convenient for high-energy amplifier chains employing difference frequency generation and/or parametric amplification stages. The technique can also serve as a way to produce pulses of ~10 fs duration throughout the visible to mid-infrared spectrum for hyperspectral ultrafast spectroscopy. Adiabatic frequency conversion employs a slowly changing position-dependent poling frequency in a chirped QPM device to efficiently frequency shift photons over a wide bandwidth with a linear transfer function. In this work, we show that the frequency dependent localized conversion of the process allows tailoring of the total group-delay dispersion (GDD). We have demonstrated a first device with zero GDD, allowing efficient conversion of a few-cycle near-infrared input to a near-single-cycle mid-infrared output of the same duration (~12 fs, with bandwidth spanning 2.0-4.0 microns). We present additional designs for precise custom tailoring of the frequency-dependent group delay.
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