Methods and systems for coherent multidimensional spectroscopy
A method for coherent multidimensional spectroscopy may comprise illuminating a location in a sample with a set of m coherent light pulses, each coherent light pulse having an initial frequency ω m and an initial wave vector {right arrow over (k)} m , wherein m≥2, to generate a coherent output signal having an initial frequency ω output =Σ±ω m and an initial wavevector wave vector {right arrow over (k)} output =Σ±{right arrow over (k)} m ; scanning a first coherent light pulse of the set of m coherent light pulses across a set of i frequency values, wherein i≥2, the set of i frequency values including the first coherent light pulse having initial frequency ω 1 ; scanning, simultaneously, a second coherent light pulse of the set of m coherent light pulses across a set of i correlated frequency values, the set of i correlated frequency values including the second coherent light pulse having initial frequency ω 2 , wherein each correlated frequency value is associated with a corresponding frequency value of the set of i frequency values as a correlated frequency grouping; and detecting the coherent output signal. Each correlated frequency value is selected so that the coherent output signal generated at each correlated frequency grouping equals the initial frequency ω output and the coherent output signal generated at each correlated frequency grouping equals the initial wavevector {right arrow over (k)} output .
1. A method for coherent multidimensional spectroscopy, the method comprising:
(a) illuminating a location in a sample with a set of m coherent light pulses, each coherent light pulse having an initial frequency ω m and an initial wave vector {right arrow over (k)} m , wherein m≥2, to generate a coherent output signal having an initial frequency ω output =Σ±ω m and an initial wave vector {right arrow over (k)} output =Σ±{right arrow over (k)} m ;
(b) scanning a first coherent light pulse of the set of m coherent light pulses across a set of i frequency values, wherein i≥2, the set of i frequency values including the first coherent light pulse having initial frequency ω 1 ;
(c) scanning, simultaneously, a second coherent light pulse of the set of m coherent light pulses across a set of i correlated frequency values, the set of i correlated frequency values including the second coherent light pulse having initial frequency ω 2 , wherein each correlated frequency value is associated with a corresponding frequency value of the set of i frequency values as a correlated frequency grouping;
wherein each correlated frequency value is selected so that the coherent output signal generated at each correlated frequency grouping equals the initial frequency ω output and the coherent output signal generated at each correlated frequency grouping equals the initial wave vector {right arrow over (k)} output ; and
(d) detecting the coherent output signal.
2. The method of claim 1 , wherein m=2 and the initial frequency is ω output =ω 1 +ω 2 and the initial wave vector is {right arrow over (k)} output ={right arrow over (k)} 1 +{right arrow over (k)} 2 .
3. The method of claim 1 , wherein m=3 and the initial frequency is ω output =±ω 1 ±ω 2 ±ω 3 and the initial wave vector is {right arrow over (k)} output =±{right arrow over (k)} 1 ±{right arrow over (k)} 2 ±{right arrow over (k)} 3 .
4. The method of claim 1 , wherein m=4 and the initial frequency is ω output =±ω 1 ±ω 2 ±ω 3 ±ω 4 and the initial wave vector is {right arrow over (k)} output =±{right arrow over (k)} 1 ±{right arrow over (k)} 2 ±{right arrow over (k)} 3 ±{right arrow over (k)} 4 .
5. The method of claim 3 , wherein the initial frequency is ω output =ω 1 −ω 2 +ω 3 and the initial wave vector is {right arrow over (k)} output ={right arrow over (k)} 1 −{right arrow over (k)} 2 +{right arrow over (k)} 3 .
6. The method of claim 3 , wherein the initial frequency is ω output =ω 1 +ω 2 +ω 3 and the initial wave vector is {right arrow over (k)} output ={right arrow over (k)} 1 +{right arrow over (k)} 2 +{right arrow over (k)} 3 .
7. The method of claim 1 , wherein angles are defined between propagation axes of each pair of coherent light pulses in the set of m coherent light pulses and the angles are fixed during steps (a)-(c).
8. The method of claim 1 , wherein step (b) is characterized by a frequency change between frequency values in the set of i frequency values and step (c) is characterized by a correlated frequency change between correlated frequency values in the set of i correlated frequency values, and further wherein the frequency change and the correlated frequency change differ in one or more of magnitude and direction.
9. The method of claim 1 , wherein the first and second coherent light pulses are collinear.
10. The method of claim 1 , further comprising
(e) scanning, simultaneously, a third coherent light pulse of the set of m coherent light pulses across a second set of i correlated frequency values, the second set of i correlated frequency values including the third coherent light pulse having initial frequency ω 3 , wherein each correlated frequency value in the second set of i correlated frequency values is also a member of the correlated frequency grouping;
wherein each correlated frequency value in the second set of i correlated frequency values is selected so that the coherent output signal generated at each correlated frequency grouping equals the initial frequency ω output and the coherent output signal generated at each correlated frequency grouping equals the initial wave vector {right arrow over (k)} output .
11. The method of claim 10 , wherein the first, the second, and the third coherent light pulses are collinear.
12. A system for coherent multidimensional spectroscopy, the system comprising:
an optical subsystem configured to illuminate a location in a sample with a set of m coherent light pulses, each coherent light pulse having an initial frequency ω m and an initial wave vector {right arrow over (k)} m , wherein m≥2, to generate a coherent output signal having an initial frequency ω output =Σ±ω m and an initial wave vector {right arrow over (k)} output =Σ±{right arrow over (k)} m ;
a detection subsystem configured to detect the coherent output signal; and
a controller comprising a processor and a non-transitory computer-readable medium operably coupled to the processor, the non-transitory computer-readable medium comprising instructions, that, when executed by the processor, cause the system to
(a) illuminate the location with the set of m coherent light pulses to generate the coherent output signal;
(b) scan a first coherent light pulse of the set of m coherent light pulses across a set of i frequency values, wherein i≥2, the set of i frequency values including the first coherent light pulse having initial frequency ω 1 ;
(c) scan, simultaneously, a second coherent light pulse of the set of m coherent light pulses across a set of i correlated frequency values, the set of i correlated frequency values including the second coherent light pulse having initial frequency ω 2 , wherein each correlated frequency value is associated with a corresponding frequency value of the set of i frequency values as a correlated frequency grouping;
wherein each correlated frequency value is selected so that the coherent output signal generated at each correlated frequency grouping equals the initial frequency ω output and the coherent output signal generated at each correlated frequency grouping equals the initial wave vector {right arrow over (k)} output ; and
(d) detect the coherent output signal.
13. The system of claim 12 , the computer-readable medium further having computer-readable instructions stored thereon that, when executed by the processor, cause the controller to generate the set of i correlated frequency values and output the set of i correlated frequency values to the system.
14. A method for coherent multidimensional spectroscopy using the system of claim 12 , the method comprising:
(a) illuminating the location with the set of m coherent light pulses to generate the coherent output signal;
(b) scanning the first coherent light pulse of the set of m coherent light pulses across the set of i frequency values;
(c) scanning, simultaneously, the second coherent light pulse of the set of m coherent light pulses across the set of i correlated frequency values; and
(d) detecting the coherent output signal.
15. A controller for controlling the operations of a system for coherent multidimensional spectroscopy, the controller comprising:
a processor; and
a non-transitory computer-readable medium operably coupled to the processor, the non-transitory computer-readable medium comprising instructions, that, when executed by the processor, cause the system to:
(a) illuminate a location in a sample with a set of m coherent light pulses, each coherent light pulse having an initial frequency ω m and an initial wave vector {right arrow over (k)} m , wherein m≥2, to generate a coherent output signal having an initial frequency ω output =Σ±ω m and an initial wave vector {right arrow over (k)} output =Σ±{right arrow over (k)} m ;
(b) scan a first coherent light pulse of the set of m coherent light pulses across a set of i frequency values, wherein i≥2, the set of i frequency values including the first coherent light pulse having initial frequency ω 1 ;
(c) scan, simultaneously, a second coherent light pulse of the set of m coherent light pulses across a set of i correlated frequency values, the set of i correlated frequency values including the second coherent light pulse having initial frequency ω 2 , wherein each correlated frequency value is associated with a corresponding frequency value of the set of i frequency values as a correlated frequency grouping;
wherein each correlated frequency value is selected so that the coherent output signal generated at each correlated frequency grouping equals the initial frequency ω output and the coherent output signal generated at each correlated frequency grouping equals the initial wave vector {right arrow over (k)} output ; and
(d) detect the coherent output signal.
16. The controller of claim 15 , the computer-readable medium further having computer-readable instructions stored thereon that, when executed by the processor, cause the controller to generate the set of i correlated frequency values and output the set of i correlated frequency values to the system.
17. A non-transitory computer-readable medium comprising computer-readable instructions stored thereon that, when executed by a processor, cause a controller for controlling the operations of a system for coherent multidimensional spectroscopy to direct the system to:
(a) illuminate a location in a sample with a set of m coherent light pulses, each coherent light pulse having an initial frequency ω m and an initial wave vector {right arrow over (k)} m , wherein m≥2, to generate a coherent output signal having an initial frequency ω output =Σ±ω m and an initial wave vector wave vector {right arrow over (k)} output =Σ±{right arrow over (k)} m ;
(b) scan a first coherent light pulse of the set of m coherent light pulses across a set of i frequency values, wherein i≥2, the set of i frequency values including the first coherent light pulse having initial frequency ω 1 ;
(c) scan, simultaneously, a second coherent light pulse of the set of m coherent light pulses across a set of i correlated frequency values, the set of i correlated frequency values including the second coherent light pulse having initial frequency ω 2 , wherein each correlated frequency value is associated with a corresponding frequency value of the set of i frequency values as a correlated frequency grouping;
wherein each correlated frequency value is selected so that the coherent output signal generated at each correlated frequency grouping equals the initial frequency ω output and the coherent output signal generated at each correlated frequency grouping equals the initial wave vector {right arrow over (k)} output ; and
(d) detect the coherent output signal.
18. The non-transitory computer-readable medium of claim 17 , further comprising instructions that, when executed by the processor, cause the controller to generate the set of i correlated frequency values and output the set of i correlated frequency values to the system.