the design of a practical detection system is predicated upon accepted theoretical principles of atomic - molecular absorption and emission which have been verified by experimental evidence . this detecting technology is also based on the principle that the emission of radiated energy , as a function of particle excursion between energy levels , is enhanced by an incident electromagnetic radiation upon the target molecular structure . that emitted radiation , which is obtained as a result of the stimulated energy level transitions at the molecular level , assumes an increased current density , which allows the explosive chemical to emit electromagnetic radiation , which can be detected by special high sensitivity detecting electronics . although the detection system was designed especially for the early detection of improvised explosive devices ( ieds ) carried by humans ( hieds ) or ieds set up remotely at roadside , or ieds that are concealed by optically opaque devices , enclosures or coverings , the system can be applied to analyze all molecular structures whether solid , liquid or in the vapor / gas phase . the emitted electromagnetic radiation that obtains from the incident radiation upon the molecular structure is referred to herein as secondary radiation . the primary emission is the incident radiation . the process is a closed loop function and is referred to here as seed , which refers to stimulated emission and enhanced detection . the incident radiation is in the thz spectrum and is utilized in such a way as to elicit secondary emission . at normal temperatures molecules are either in their ground state or in their low - lying excited states . if an incident radiation presented to the atomic - molecular structure is large with respect to the size of the structure ( nucleus ) scattering occurs . the scattering which occurs , in this particular case , can be described in terms of classical electromagnetic theory . this particular scattering is referred to as rayleigh scattering . the probability of rayleigh scattering varies inversely as the fourth power of the wavelength ( ρ λ = 1 / λ 4 ) and thus increases with the fourth power of frequency ( ρ f = f 4 ). various other scattering principles are applied in the detection methodology described herein . electromagnetic radiation refers to the composite transmission of a mutually perpendicular electric and magnetic fields of some relative energy . energy in the electromagnetic field is comprised of discrete units , which have been described as photons . when an electromagnetic field is incident on a molecule most of these photons are elastically scattered , having the same energy and wavelength as the incident photons . but about one photon out of every 10 7 ( ten million ) photons are inelastically scattered and produce wavelengths that are different from the wavelength incident on the molecular structure ; usually they are longer in wavelength than the incident ray . that process which describes inelastic scattering is referred to here as raman scattering . raman scattering can occur with a change in the vibrational , rotational or electronic energy of a molecule . the difference between the energy of the incident photon and the raman photon is equal to the vibrational energy of the scattering molecule . the raman spectrum is constructed from the intensity of the scattered emission compared to the energy difference . several embodiments of the present system utilizes raman scattering . thus , when the incident photon interacts with the electric dipole of the molecule , the resulting emissions constitute the raman effect . in terms of classical physics , that interaction would be described as a perturbation of the molecular electric field . however , in quantum physics , the raman scattering effect refers to the effect of a particle excursion to an altered state of excitation energy ; thus having coincident lower excitation with a change in vibrational energy that corresponds to the energy differential . raman scattering , therefore , applies directly to embodiments of the present invention for the early detection of improvised explosive devices ( ieds ). the general principles of rayleigh and mie scattering also apply to some extent and are presented for continuity and clarity of explanation . the quantum discussion as well as the classical discussion , here , is important to understanding the theoretical basis for the claimed methodology of early detection . the discussion begins by recognizing that raman scattering refers to inelastic scattering . however , both inelastic scattering and elastic scattering are germane to the present discussion . inelastic scattering occurs when the incident photon has sufficient kinetic energy to cause an atom to transition from a lower state of excitation energy to a higher state of excitation energy . elastic scattering occurs when the target molecule has sufficient mass as to appear as though infinite with respect to a projectile particle . the energy of the scattered photon is related to the incident energy of the photon which is given in terms of hf where : hf ′= hf − δe , and where δe is the excitation energy that describes the difference between the higher excitation state and the ground state ; h is plank &# 39 ; s constant and f is frequency . the energy and , therefore , the frequency or wavelength of the scattered radiation is altered as the radiation either imparts rotational or vibrational energy to the scattering molecules or subtracts energy . the line spectrum of the scattered emissions will have one prominent line corresponding to the original wavelength of the incident radiation and additional lines on each side of it . these additional lines correspond to the shorter or longer wavelengths of the altered portion of the radiation spectrum . it is this raman spectrum that is characteristic of the transmitting molecular substance ( the molecular structure ). it is particularly useful for the signature characterization of materials , which is determined by this design , in addition to the detection and confirmation of an explosive material . the iterations of the absorption - emission process described here are sometimes referred to as “ resonance absorption .” as an atom transitions from a higher energy state to a lower energy state the resulting emission of photons is referred to as spontaneous emission . this applies directly to various embodiments of the early detection methodology discussed in this document . it is the current density of the emissions that is intentionally increased with the seed methodology for purpose of detection . the increased current density facilitates higher signal to noise ratio and thus a more efficacious detection and reception process . referring now to the figures , wherein like references identify like elements of the invention , fig1 illustrates an exemplary embodiment of the invention . a backward wave oscillator 1 functions as a thz oscillator in order to establish the conditions for excitation of the target molecular compounds . it is powered by the high voltage circuit 2 . a power supply , depicted in fig3 b , 4 , 5 a and 5 b , output affects the wavelength and amplitude of the backward wave oscillator 1 . in order to amplify the thz signal generated by the backward wave oscillator 1 , a waveguide 6 is necessary to propagate the low level oscillator signal to the excitation amplifier 28 . an excitation amplifier 28 produces a high power thz emission that mitigates atmospheric aberration that would normally limit effective range . therefore , the efficacy of the excitation is a function of output power by the thz amplifier . since the thz wavelengths are short enough to be highly directional , a mechanical sweep of the antenna 9 will locate randomly placed chemical and chemical compounds . in one embodiment of the invention , a horn antenna 9 is swept across a field of motion to excite randomly located molecules , whereupon the detection results from the collapsing energy state of the molecular compound back to its ground state . the excitation of target molecules depends not only on the output power of the thz signal but also on the modulation , which is utilized to find resonance with the molecular transitions as well as the inherent molecular resonance . in one embodiment , the modulation is accomplished by the operation of modulated thz radiation output 13 , a feedback detector 14 , a digital signal processor 12 , a pulse / phase generator 11 , and a pulse / phase modulator 10 as depicted in fig1 . in several embodiments , the modulation is a critical factor and unique to this invention . it is a method by which resonance with the molecular compound is achieved . the repetition rates and the pulse width and the phase angle of a sinusoidal emission are developed to resonate with the sub harmonics and transition states of the molecular compound . in some exemplary embodiments , a main computer 18 is a host manager that delegates the actual real - time operation down to digital signal processors 5 , 12 . the main computer 18 performs database management which allows the dedicated digital signal processors 5 , 12 to perform at higher speeds . in another embodiment , a power amplifier 28 requires a high voltage , high current power supply . a thz power supply 15 powers both the backward wave oscillator 1 and the power output tube of the thz power amplifier 28 . a common transformer t 401 supports two rectifier circuits depicted in fig4 . posts hv1 common and hv1 + apply to the backwards wave oscillator 1 . posts labeled hv2 common and hv2 + apply to the power amplifier 28 . the transformer t 401 operates at 100 khz . by increasing the operating frequency the magnetics are reduced substantially . therefore the size and weight of the power supply are reduced also . a series of circuits depicted in fig3 a , fig3 b , fig5 a , fig5 b , and fig4 allow the power supplies to operate at 100 khz instead of 60 hz . the power output is controlled in a closed loop fashion according the algorithms in a digital signal processor 12 and also by the feedback loop configured by the digital signal processor 12 , a modulated thz radiation output 13 , a feedback detector 14 , and a thz power supply 15 . in this embodiment , the main computer 18 will initiate as much iteration as needed to confirm the valid detection of a molecular compound and assess its characteristic properties . the data collected by the main computer 18 is added to the database in order to build a table of properties relating to the molecular compounds analyzed . the information is compared to a table of raman spectral data . in the case of buried or optically obscured chemicals or chemical compounds , primary detection rests on the thz carrier because ir is constrained by the principles of optics . in laboratories and other such places the application of raman spectroscopy becomes efficacious due to the advantage of close proximity and humidity control . the application of raman spectroscopy for analysis is feasible and is included instrumentally in the apparatus described herein . the diversity of ied tactical circumstances , especially related to techniques to obscure detection strongly suggests the use of thz for all possible scenarios . the problem of excitation at standoff distances by this method together with the modulation and appropriate power enables practical early detection . this method facilitates the process of stimulated emission , which is also referred to as secondary emission in this document . when the molecular structure is alternately excited and collapsed by oscillating excitation pulses , determined according to the modulation algorithm , emission from the excited - ground state transitions must be sufficient for practical detection . to facilitate detection the specific circumstances of the emission to be detected must be resolved . the emission of interest will be electromagnetic radiation at some defined spectral segment in either the infrared spectrum or the terahertz spectrum or both , and at some very low level of intensity . the level of intensity is a major concern since normal emission intensities are of insufficient amplitude to be detected at any significant distance , and they are obscured beneath the noise amplitudes . therefore , normal stimulated emission amplitudes are impractical for detection . increasing the amplification factor of the detecting system will also increase the noise amplitude , thus retaining the original problematic signal to noise ratio ( snr ) making detection impractical . what is required is ( 1 ) sufficient signal amplitude for remote detection , and ( 2 ) a favorable signal to noise ratio prior to detection . the amplitude of the stimulated emission is not entirely a function of the power applied to the excitation process but rather a function of the current density of the emission itself , which is determined by the transition of energy states and the molecular structure . by modulating the excitation in such a way as to modify the rate of change of energy states with respect to time , one thus increases the total current density of the emission . since current density is a function of the excursion between energy levels ( δε ), a given current density per transition ( δε ) can be defined . the modulation yields f ( i )=∫ f ( ε )· di . the total area under the curve represents current density . by this method , the current density of the stimulated emission is increased by remote methods . thus , the snr is also increased significantly by increasing the current density and , therefore , the signal amplitude is increased beyond the noise amplitude . there is , of course , a maximum amplitude level of current density that is uniquely associated with a given molecular structure . a distribution of maximum attainable current densities for a given set of molecular configurations can be constructed . once detection has been captured the objective is how to discern the emission of interest from some spurious emission . there must be certitude regarding the detection of an ied . the function here is closed loop processing . a modulation algorithm transmitted is compared with a detected algorithm for agreement for this purpose . for example , if a series of transmissions for excitation are followed at intervals with some function , say 977mod ( x )+ 135mod ( y )= n , the system will determine that n is , say 6 , for instance , and the capture will be valid . any other number besides 6 will reject the capture as a spurious reception . more accurately , one says f ( u ) mod ( u )+ f ( v ) mod ( v )= n . however , the process is rapidly iterated and a voting scheme similar to that used in fighter jets and spacecraft is employed . achieved thereby is ( 1 ) excitation of the explosive material , ( 2 ) improved detectability by increasing the current density of the stimulated emission , and ( 3 ) determination of a valid or non - valid conditional response . various embodiments of the present invention thus can be used to detect , locate , and identify chemicals and chemical compounds including but not limited to explosive molecular compounds such as those used in ieds . it may also be used to detect , locate , and identify organic and inorganic explosives including precursors , chemical warfare agents including precursors , pesticides , narcotics , solvents , and naturally occurring toxins to include the examination of materials having inhomogeneous compositions . embodiments of the invention makes particular use of seed to provide longer standoff distances while avoiding the adverse impacts of atmospheric disturbances . depending on the configuration of the elements described herein , the standoff distance can be 10 meters , 25 meters , 50 meters , 100 meters , 250 meters , or greater . thus , it should be understood that the embodiments and examples have been chosen and described in order to best illustrate the principals of the invention and its practical applications to thereby enable one of ordinary skill in the art to best utilize the invention in various embodiments and with various modifications as are suited for particular uses contemplated . even though specific embodiments of this invention have been described , they are not to be taken as exhaustive . there are several variations that will be apparent to those skilled in the art .