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A low degree of temporal coherence can also be beneficial for laser projection displays, imaging and pointer applications, as it reduces the tendency for laser speckle and similar interference effects.

In situations where only a single resonator mode has sufficient laser gain to oscillate, a single longitudinal mode can be selected, obtaining single-frequency operation with very high temporal coherence as well. Using additional techniques for stabilizing the frequency, the linewidth can be further reduced to a massive extent. Some laser systems serve as optical frequency standards with a linewidth below 1 Hz, which implies an extremely high temporal coherence and a coherence length of hundreds of thousands of kilometers.

These explain quite comprehensively a wide range of aspects, not only physical principles of operation, but also various practical issues.

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Some applications need laser light with very high spatial and temporal coherence. This applies, e.g., to many variations of interferometry, holography, and some types of optical sensors (e.g. fiber-optic sensors). Such features are also important for the technique of coherent beam combining.

In quantum optics, the term coherence is often used for the state of light-emitting atoms or ions. In that case, coherence refers to a phase relationship between the complex amplitudes corresponding to electronic states. This is important, e.g., in the context of lasing without inversion.

For other applications, the coherence of the light used should be as low as possible. For example, very low temporal coherence (but combined with high spatial coherence) is required for optical coherence tomography, where images are created with a kind of interferometry, and a high spatial resolution requires low temporal coherence. Suitable light sources for such applications can be based on amplified spontaneous emission (ASE) from a laser amplifier (→ superluminescent sources) or on supercontinuum generation in nonlinear media.

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Figure 4 shows a laser beam with reduced spatial coherence, but high temporal coherence. The wavefronts are deformed, and this results in a high beam divergence and poor beam quality. On the other hand, the beam is monochromatic, so that the spacing of the deformed wavefronts remains constant. Such a beam can result from a single-frequency laser, when its output is sent through some optically inhomogeneous material.

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Figures 2–4 further illustrate the difference between spatial and temporal coherence. For reference, Figure 2 shows a monochromatic Gaussian beam, exhibiting perfect spatial and temporal coherence.

Lasers have the potential for generating beams (e.g. Gaussian beams) with very high spatial coherence, and this is perhaps the most fundamental difference between laser light and radiation from other light sources. High spatial coherence of laser light arises from the existence of resonator modes, which define spatially correlated field patterns.

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See also the discussion on the coherence of supercontinua, and the article concerning coherence of ultrashort pulses in the Photonics Spotlight.

Figure 3 shows a beam with high spatial coherence, but poor temporal coherence. The wavefronts are formed as above, and the beam quality is still very high, but the amplitude and phase of the beam varies along the propagation direction. Note that both the local amplitude and the spacing of the wavefronts vary to some extent. Such a beam can be generated e.g. from the output of a supercontinuum source.

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It is also common to call certain processes or techniques coherent or incoherent. In that case, “coherent” essentially means phase-sensitive. For example, the general method of coherent beam combining relies on the mutual coherence of beams, whereas spectral (incoherent) beam combining does not

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Partial coherence means that there is some (although not perfect) correlation between phase values. There are various ways of quantifying the degree of coherence, as described below.

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Quantitative specifications of coherence may result from theoretical calculations (involving statistical methods) or from measurements. In most cases, measurements involve some kind of interference. For example, one may measure the interference contrast as a function of path length difference to get a correlation function.

A special case are lasers for ultrashort pulses, where the relationship between optical bandwidth and temporal coherence is non-trivial. A pulse train from a mode-locked laser can have a broad overall bandwidth, with the Fourier spectrum consisting of discrete very narrow lines (→ frequency combs). The temporal coherence can be very high in the sense that there are strong field correlations for large time delays which are close to integer multiples of the pulse period.

There is not a single universal technique to measure laser linewidths or coherence lengths. Different setups are employed for different linewidth regimes. See our application note on coherence issues.

Coherence is one of the most important concepts in optics and is strongly related to the ability of light to exhibit interference effects. A light field is called coherent when there is a fixed phase relationship between the electric field values at different locations or at different times.

If a laser beam with high spatial coherence is sent through an optical diffuser element (for example, a very inhomogeneous piece of glass) which totally scrambles the wavefront, the resulting distorted beam could in principle still be considered as spatially coherent, since the phase relationship between the electric fields at different points would still be fixed, as long as the wavefront distortions do not change with time. It would then also in principle be possible to restore a simple beam shape by applying another optical element which compensates the complicated spatial distortions. For most practical purposes, however, such a distorted beam will be spatially incoherent. Nevertheless, a real destruction of spatial coherence requires time-dependent wavefront distortions, as can be obtained with a rotating diffuser, for example. In that case, the temporal coherence is also somewhat degraded, while it would be completely preserved if only a stationary diffuser is used.

On the other hand, many lasers emit on multiple modes with substantially different optical frequencies, and their temporal coherence is correspondingly low. Even for single-frequency lasers, the temporal coherence can be weak due to strong phase noise. That is often observed in laser diodes, for example.