量子效率

It has direct drive with no backlash and can microstep in the sub-nano millimeter range. The motor comes as three different versions; standard stainless steel for normal environment, a vacuum version and a non-magnetic vacuum version.

Solar panelefficiency

When your application requires higher than 40N operational force or if you wish to have direct rotary drive, then please reach out to us, we have other solutions for you

Photoelectric conversionefficiency

The Legs Linear LL06 Piezo Motor has direct drive with no backlash and can microstep in the sub-nano meter range. It weighs only 16 grams and has a stall force of 6.5N. It is available with built-in encoder.

In optical spectroscopy, the quantum yield is the probability that a given quantum state is formed from the system initially prepared in some other quantum state. For example, a singlet to triplet transition quantum yield is the fraction of molecules that, after being photoexcited into a singlet state, cross over to the triplet state.

Spectral response

Φ = #   m o l e c u l e s   d e c o m p o s e d #   p h o t o n s   a b s o r b e d {\displaystyle \Phi ={\frac {\rm {\#\ molecules\ decomposed}}{\rm {\#\ photons\ absorbed}}}}

It has direct drive with no backlash and can microstep in the sub-nano millimeter range. The motor comes as three different versions; standard stainless steel for normal environment, a vacuum version and a non-magnetic vacuum version.

The quantum yield of a photochemical reaction describes the number of molecules undergoing a photochemical event per absorbed photon:[1]

In a chemical photodegradation process, when a molecule dissociates after absorbing a light quantum, the quantum yield is the number of destroyed molecules divided by the number of photons absorbed by the system. Since not all photons are absorbed productively, the typical quantum yield will be less than 1.

Fluorescence quantum yield is measured on a scale from 0 to 1.0, but is often represented as a percentage. A quantum yield of 1.0 (100%) describes a process where each photon absorbed results in a photon emitted. Substances with the largest quantum yields, such as rhodamines, display the brightest emissions; however, compounds with quantum yields of 0.10 are still considered quite fluorescent.

Internalquantum efficiency

Quantum yields of photochemical reactions can be highly dependent on the structure, proximity and concentration of the reactive chromophores, the type of solvent environment as well as the wavelength of the incident light. Such effects can be studied with wavelength-tunable lasers and the resulting quantum yield data can help predict conversion and selectivity of photochemical reactions.[11]

If you want to know more about the technology, please visit our Piezo Motor Technology page. Our How to Achieve High Precision Motion Page gives insights on various motion and motor techniques.

Experimentally, relative fluorescence quantum yields can be determined by measuring fluorescence of a fluorophore of known quantum yield with the same experimental parameters (excitation wavelength, slit widths, photomultiplier voltage etc.) as the substance in question. The quantum yield is then calculated by:

In particle physics, the quantum yield (denoted Φ) of a radiation-induced process is the number of times a specific event occurs per photon absorbed by the system.[1]

Φ = #   m o l e c u l e s   u n d e r g o i n g   r e a c t i o n   o f   i n t e r e s t #   p h o t o n s   a b s o r b e d   b y   p h o t o r e a c t i v e   s u b s t a n c e {\displaystyle \Phi ={\frac {\rm {\#\ molecules\ undergoing\ reaction\ of\ interest}}{\rm {\#\ photons\ absorbed\ by\ photoreactive\ substance}}}}

Φ = Φ R × I n t I n t R × 1 − 10 − A R 1 − 10 − A × n 2 n R 2 {\displaystyle \Phi =\Phi _{\mathrm {R} }\times {\frac {\mathit {Int}}{{\mathit {Int}}_{\mathrm {R} }}}\times {\frac {1-10^{-A_{\mathrm {R} }}}{1-10^{-A}}}\times {\frac {{n}^{2}}{{n_{\mathrm {R} }}^{2}}}}

Externalquantum efficiency

Fluorescence quantum yields are measured by comparison to a standard of known quantum yield.[2] The quinine salt quinine sulfate in a sulfuric acid solution was regarded as the most common fluorescence standard,[3] however, a recent study revealed that the fluorescence quantum yield of this solution is strongly affected by the temperature, and should no longer be used as the standard solution. The quinine in 0.1M perchloric acid (Φ = 0.60) shows no temperature dependence up to 45 °C, therefore it can be considered as a reliable standard solution.[4]

The subscript R denotes the respective values of the reference substance.[5][6] The determination of fluorescence quantum yields in scattering media requires additional considerations and corrections.[7]

Förster resonance energy transfer efficiency (E) is the quantum yield of the energy-transfer transition, i.e. the probability of the energy-transfer event occurring per donor excitation event:

A fluorophore's environment can impact quantum yield, usually resulting from changes in the rates of non-radiative decay.[2] Many fluorophores used to label macromolecules are sensitive to solvent polarity. The class of 8-anilinonaphthalene-1-sulfonic acid (ANS) probe molecules are essentially non-fluorescent when in aqueous solution, but become highly fluorescent in nonpolar solvents or when bound to proteins and membranes. The quantum yield of ANS is ~0.002 in aqueous buffer, but near 0.4 when bound to serum albumin.

The fluorescence quantum yield is defined as the ratio of the number of photons emitted to the number of photons absorbed.[2]

Detectivequantum efficiency

Φ = μ m o l   C O 2   f i x e d μ m o l   p h o t o n s   a b s o r b e d {\displaystyle \Phi ={\frac {\rm {\mu mol\ CO_{2}\ fixed}}{\rm {\mu mol\ photons\ absorbed}}}}

E = Φ F R E T = k E T k E T + k f + ∑ k n r {\displaystyle E=\Phi _{\mathrm {FRET} }={\frac {k_{\mathrm {ET} }}{k_{\mathrm {ET} }+k_{f}+\sum k_{\mathrm {nr} }}}}

Linear actuators based on our Piezo LEGS proprietary technology are developed and manufactured in house Our standard range include 6.5 – 40N linear motors.  Our custom range include motors up to 450N and rotary piezo motors. Use our Linear Actuator Configurator to easily find a complete and nicely priced Starter Kit.

quantumefficiency中文

Non-radiative processes are excited state decay mechanisms other than photon emission, which include: Förster resonance energy transfer, internal conversion, external conversion, and intersystem crossing. Thus, the fluorescence quantum yield is affected if the rate of any non-radiative pathway changes. The quantum yield can be close to unity if the non-radiative decay rate is much smaller than the rate of radiative decay, that is kf > knr.[2]

Full force power-off locking is a safety function inherent to the design. A version of the motor, designed for vacuum and non-magnetic environments, is available.

Φ ( λ ) =  number of events   number of photons absorbed  {\displaystyle \Phi (\lambda )={\frac {\text{ number of events }}{\text{ number of photons absorbed }}}}

Quantum yields greater than 1 are possible for photo-induced or radiation-induced chain reactions, in which a single photon may trigger a long chain of transformations. One example is the reaction of hydrogen with chlorine, in which as many as 106 molecules of hydrogen chloride can be formed per quantum of blue light absorbed.[10]

Φ = #   p h o t o n s   e m i t t e d #   p h o t o n s   a b s o r b e d {\displaystyle \Phi ={\frac {\rm {\#\ photons\ emitted}}{\rm {\#\ photons\ absorbed}}}}