A detailed explanation of mid-infrared fibers and their applications

Ultra-fast pulse tuning frequency conversion based on hollow core fibers

There are several types of hollow core fibers: band gap, negative curvature and Bragg cladding. Regardless of the type, the preparation process is complex. Many people would also question the application of hollow core fibers, considering them too heavy and immature. However, this technology, which conceals new physical phenomena, offers a rare environment for many experiments. Today we present tunable frequency conversion of ultrafast pulses based on optical fibers. Using a drawn hollow fiber filled with nitrogen, ultrafast 1 μm laser pulses can be tunably converted to longer wavelengths and shorter pulse times.

In this conceptual diagram, the ultrafast laser pulse (blue) on the left enters a stretched hollow-core fiber filled with nitrogen (red molecules) and, as it propagates, obtains a spectral broadening, with the output beam (orange) on the right. This nonlinear phenomenon is due to the Raman effect, which is linked to the rotation of gas molecules in the laser field.

Yb fiber lasers can produce ultrafast pulses with a central wavelength of about 1 μm, but in many applications (e.g., high harmonic generation, OCT optical coherence tomography in medicine), Ultrafast pulses with high energy and slightly longer wavelength are required. ). Conventional sources of wavelength-tunable ultrafast pulses, optical parametric amplifiers (OPAs), convert ultrafast 1 μm pulses to frequency and allow continuous tuning from 1,3 to 4,5 μm, although the range of 1,0-1,3 μm cannot be achieved without additional frequencies. Additionally, takeover bids are generally complex and expensive to construct.  

Here we present a simpler method that can generate ultrafast pulses in the 1-1,7 μm region: a 1 μm pump pulse is sent along a long nitrogen-filled channel section in a fiber at hollow core, which results in an extreme Raman shift (extreme Raman red-shifTIng) of the light. An additional advantage of this method is the reduction of the pulse from 200 fs to around 20 fs. 

How is it possible ?

(A)

(1) Compare this method to conventional experiments in which a hollow core fiber is typically filled with a monatomic gas (e.g. argon) to symmetrically expand the laser spectrum and then recompress it into a short pulse.

(2) In this experiment, the team found that by using, for example, nitrogen, it was still possible to broaden the spectrum, but in an unexpected asymmetric way.  

The beam is broadened towards long infrared (IR) wavelengths, allowing the output spectrum to be filtered to retain the band where it is to be applied. In this way, the energy is transmitted in the near infrared spectral range with a pulse three times shorter (which makes it possible to obtain an efficiency comparable to that of OPA); and most importantly, the process does not require complex equipment or additional pulse post-compression systems.  

(B) Another experiment: the team used a hollow-core fiber filled with nitrogen and, instead of filtering the spectrum, compressed it in time using a dispersive lens capable of adjusting the phase of the expanded pulse. strong field physics (attosecond and strong field physics)”.  

(C) Stretching a hollow core fiber (HCF) and then pumping a 200 fs, 1,03 μm pulse from an amplified Yb-based laser system. TUWien's device uses a fiber 5,5 m long and 1 mm in internal diameter; INRS uses a fiber 6 m long and 0,53 mm in internal diameter, as well as broadband chirped mirrors to compress the pulses.  

The Moscow group, led by Aleksei ZhelTIkov, focuses on developing theoretical models to explain these optical phenomena. By combining these three approaches, the researchers were able to not only fully understand the complex underlying dynamics, but also use nitrogen to achieve extreme red shift and effective pulse compression in the infrared region. effective compression of pulses in the infrared range).  

The team believes that a Raman shift-based approach could well meet the growing demand for longer-wavelength ultrafast light sources for laser and strong-field applications, starting with cheaper, tunable systems. industrial quality.

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