Optical devices
US-11867562-B2 · Jan 9, 2024 · US
US10436650B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10436650-B2 |
| Application number | US-201414781382-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 1, 2014 |
| Priority date | Apr 2, 2013 |
| Publication date | Oct 8, 2019 |
| Grant date | Oct 8, 2019 |
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An approach to nanoscale thermometry that utilizes coherent manipulation of the electronic spin associated with nitrogen-vacancy (NV) color centers in diamond is disclosed. The methods and apparatus allow for detection of temperature variations down to milli-Kelvin resolution, at nanometer length scales. This biologically compatible approach to thermometry offers superior temperature sensitivity and reproducibility with a reduced measurement time. The disclosed apparatus can be used to study heat-generating intracellular processes.
Opening claim text (preview).
What is claimed is: 1. A method of measuring temperature of a heat source comprising: providing an electron spin system comprising a diamond NV center proximal to the heat source, said diamond NV center having a temperature-dependent zero-field splitting of its ground electronic spin state; applying an optical pulse to polarize the ground electronic spin state; applying a plurality of microwave pulses to alter the spin population of the spin system; applying a series of optical pulses to the spin system; measuring a spin-state-dependent fluorescence rate to detect the spin projection of the electronic ground state of the NV center; and determining the temperature of the heat source from the spin-state-dependent fluorescence rate. 2. The method of claim 1 , wherein the determined temperature is indicative of a temperature at the micro to nanometer scale. 3. The method of claim 1 , wherein the plurality of microwave pulses comprises a 2π-echo-pulse sequence or its equivalent variations. 4. The method of claim 1 wherein the microwave pulse is detuned from the zero-field splitting by 0 MHz to 500 MHz of the resonant frequency. 5. The method of claim 1 , wherein the evolution time is in the range of 0 μs to 10000 μs. 6. The method of claim 1 , wherein the temperature sensitivity ranges from 10 K/Hz 1/2 to 50 μK/Hz 1/2 . 7. The method of claim 1 , wherein the heat source has a temperature between 100K and 600K. 8. The method of claim 1 , wherein the amount of 13 C impurity in the diamond is 0.0001% to 1.2%. 9. The method of claim 1 , wherein the determining the temperature from the spin-state-dependent fluorescence rate comprises: determining temperature-dependent zero-field splitting of the NV center; and determining the temperature based on the temperature-dependent zero-field splitting.
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