Low Energy Laser Spectroscopy LELS

Abstract

An extremely sensitive spectroscopy method utilizes a laser modified to an extremely low emission with an integrated control system, interfaced within a typical Raman platform to comprise low energy laser spectroscopy (LELS). LELS acquires and utilizes a quantum entangled state of photons and particles, including omnipresent cosmological dark matter particles (OCDM) and omnipresent cosmological dark energy (OCDE). The OCDM and OCDE matter has an affinity to particles of same OCDM and OCDE matter in target specimens, with same-time data results of high sensitivity. In a semiconductor light emitter, electron flow at a low energy level is provided to a quantum well to produce a quantum tunneling of electrons into an active region of the laser quantum well and creating sublasering. Sublasering allows OCDM and OCDE to become entangled with other particles and energies in the laser's quantum well and create a transmission package comprising quantum entangled fields, waves, wave packages, states and energies. Providing a triggering pulse causes a second tunneling, carrying the transmission package for emission.

1 . A spectroscopy apparatus comprising:
 a. a quantum well diode laser;   b. a p-type layer and an n-type layer in said quantum well diode laser comprising an N-P semiconductor and having an active region intermediate the n-type layer and the p-type layer and a region extending into said n-type layer and said p-type layer, the active region including a quantum well, the quantum well comprising a region of quantum tunneling and weak diode effect;   c. an adjustable power supply comprising a source of electron flow coupled to said N-P semiconductor, and further comprising an external trigger source, the electron flow energizing said N-P semiconductor to a first, low energy level to produce a sublasering energy level, and producing visible photons wherein the bias changes the active region in the quantum well;   d. a timing circuit establishing a time interval during which the electron flow having the first, low energy level is applied to said N-P semiconductor, whereby a transmission package is formed in said quantum well comprising photons, OCDE and OCDM in quantum entanglement;   e. an external trigger coupled to trigger lasing of said quantum well diode laser to initiate transmission of the laser beam and the transmission package from said laser at a time after initiation of electron flow at the first, low energy level from said source of electron flow; and   f. a Raman probe positioned to direct the transmission package in a first direction and to receive emissions from only the first direction, whereby said probe is positioned to avoid reception of Raman photon scatter, said Raman probe having an excitation fiber, said Raman probe coupling received emissions to a spectrometer, wherein focusing is provided by a probe lens.   
     
     
         2 . The spectroscopy apparatus according to  claim 1  further comprising the spectrometer. 
     
     
         3 . The spectroscopy apparatus according to  claim 2  wherein said spectrograph input and spectrograph output are provided continuously, whereby the spectrograph is operated without time gating. 
     
     
         4 . The spectroscopy apparatus according to  claim 3  further comprising a single fiber optic strand having a first end at an interface with said Raman probe, and coupling transmitted and received energies, waves, and particles between the Raman probe interface and an opposite end of said fiber. 
     
     
         5 . The spectroscopy apparatus according to  claim 4  further comprising a mechanical coupling supporting the first end of said single fiber optic strand at a preselected location with respect to the Raman probe. 
     
     
         6 . The spectroscopy apparatus according to  claim 5  wherein said first end of said fiber is located in a convergence field of said Raman probe such that a lens at the first end of said single fiber optic strand acts as a focusing lens. 
     
     
         7 . The spectroscopy apparatus according to  claim 6  further comprising a syringe structure and wherein said single fiber optic strand is supported in said syringe structure. 
     
     
         8 . The spectroscopy apparatus according to  claim 7  wherein said syringe structure includes said mechanical coupling and wherein said mechanical coupling comprises an alignment stop and wherein an axial end of said Raman probe is positioned to rest on said alignment stop. 
     
     
         9 . The spectroscopy apparatus according to  claim 8  further comprising a time gated CCD photomultiplier and a computer interface providing time gating signals to said time gated CCD photomultiplier, wherein said time gated CCD photomultiplier is coupled to receive an output of said spectrograph, the CCD time gated photomultiplier providing an input to said source of electron flow to initiate triggering lasing. 
     
     
         10 . The spectroscopy apparatus according to  claim 1  wherein said p-type layer and said n-type layer each comprise two layers and wherein an n-type layer and an adjacent p-type layer comprise a separate confinement laser quantum well. 
     
     
         11 . The spectroscopy apparatus according to  claim 10  wherein said Raman probe is coupled to receive an input from said laser and wherein said Raman probe couples an output to a collection fiber transmitting the emission package to a spectrometer. 
     
     
         12 . A spectroscopy apparatus comprising:
 a. a transmission package generator comprising a quantum well diode laser;   b. said quantum well diode laser comprising an N-P semiconductor including an active region, the active region including a quantum well, the quantum well comprising a region of quantum tunneling and weak diode effect;   c. an adjustable power supply comprising a source coupled to said N-P semiconductor for energizing said quantum well diode laser at a first, low energy to produce sublasering in which visible photons are produced, said adjustable power supply further comprising an external trigger;   d. an adjustable power supply providing an electron flow having the first, low energy level applied to said N-P semiconductor, whereby a transmission package is formed in said quantum well, the transmission package comprising entities in quantum entanglement with a laser beam, said transmission package having the property that photons become disentangled upon entering a sample;   e. a Q-switched laser trigger pulse source coupled from said adjustable power supply to trigger lasing of said quantum well diode laser to initiate transmission of the laser beam and the transmission package; and   f. a Raman probe positioned to direct the transmission package in a first direction and to receive emissions from only the first direction, said Raman probe positioned to receive the transmission package and to collect spectral emissions, whereby said Raman probe is enabled to respond to entities which are free of photons.   
     
     
         13 . The spectroscopy apparatus according to  claim 12  further comprising:
 a. a spectrometer coupled to receive inputs from said Raman probe; 
 b. a CCD photomultiplier sensing impact of entities free of photons received in said spectrometer; 
 c. a computer coupled to said CCD photomultiplier to produce a computer-generated spectral analysis; and 
 d. said CCD photomultiplier providing a signal for initiating the laser trigger pulse, said signal comprising a change in impedance coupled to said adjustable power supply. 
 
     
     
         14 . The spectroscopy apparatus according to  claim 13  further comprising a control input for said CCD photomultiplier. 
     
     
         15 . The spectroscopy apparatus according to  claim 14  wherein said CCD photomultiplier is connected to said adjustable power supply. 
     
     
         16 . The spectroscopy apparatus according to  claim 15  further comprising a single fiber optic strand having said Raman probe coupling transmitted and received energy between the focal convergence field of said Raman probe and an opposite end of said single fiber optic strand, and a mechanical coupling supporting the first end of said single fiber optic strand at a preselected location with respect to the convergence field. 
     
     
         17 . A spectroscopy apparatus including a source of a transmission package, said source comprising:
 a. a quantum well laser diode;   b. a quantum well in said quantum well laser diode having a P-N junction defining said quantum well;   c. an adjustable power supply separate from a pre-pumping source and biasing said laser for sublasing and producing visible photons, said quantum well producing a transmission package comprising OCDE and OCDM;   d. a laser trigger pulse source for initiation of a laser beam, said laser beam comprising the transmission package;   e. a Raman probe comprising a transmission fiber and a collection fiber; and   f. said Raman probe being positioned to direct the transmission package in a first direction and to receive emissions from only the first direction.   
     
     
         18 . The spectroscopy apparatus according to  claim 17  comprising a single fiber optic strand having a first end at a focal convergence field of said Raman probe coupling transmitted and received energy between the focal convergence field of said Raman probe and an opposite end of said single fiber optic strand, and a mechanical coupling supporting the first end of said single fiber optic strand at a preselected location with respect to the convergence field. 
     
     
         19 . The spectroscopy apparatus according to  claim 17  wherein the first end of said single fiber optic strand is located within the convergence field. 
     
     
         20 . The spectroscopy apparatus according to  claim 19  wherein said single fiber optic strand is releasably secured to said Raman probe.