although specific embodiments of the invention will now be described with reference to the drawings , it should be understood that such embodiments are by way of example only and are merely illustrative of but a small number of the many possible specific embodiments to which the principles of the invention may be applied . various changes and modifications obvious to one skilled in the art to which the invention pertains are deemed to be within the spirit , scope and contemplation of the invention as further defined in the appended claims . 1 . synopsis of the invention and the preferred new optical memory materials for the case of organic photochromic memory materials the binary codes , 0 and 1 , are formed by the photo - chemical changes which lead to two distinct molecular forms with different structures . the write form of the memory material is usually colorless and absorbs light in the uv region or the spectrum . the absorption of light by this form induces a photochemical reaction , which leads to formation of the written , colored form with the absorption spectrum shifted to the visible region . accessing of information is based on the ( i ) detection of fluorescence emitted by the written bits , or ( ii ) absorption or index of refraction change . another means of writing is to use a memory material that is initially fluorescing and to radiatively induce the non - fluorescing state . in such a case the initial , fluorescing , state would commonly be defined as binary “ 0 ” while the written , non - fluorescing , state would be defined as a binary “ 1 ”. in the present invention a new memory material was designed for rom ( read only memory ) or worm ( write - once read - many ) devices , where the information should be written once , stored indefinitely , but may be retrieved an unlimited number of times . the new material is composed of an organic dye which has different structures when dispersed in acidic or basic host media . it is known , that some organic dyes , such as , for example rhodamine , may exist in two forms , depending on acidity and polarity of the matrix or solvent . one of these forms , rhodamine b base , is colorless and shows complete lack of fluorescence . however , in the presence of acid , this colorless form undergoes transformation into a colored , strongly fluorescing dye , rhodamine b , which is well known as a stable and efficient laser dye . using molecules , which have these and other similar properties , the present invention contemplates new optical storage materials , which are composed of two components : ( 1 ) a molecule , which when excited is converted into an acid or a base , radical or ion ( referred to as an acid or base , radical or ion generator ); and ( 2 ) an organic dye precursor , which reacts with the photo - generated acid , base , ion , or excited - state molecule to form a room - temperature stable , strongly - fluorescing dye . the written form of this memory material is the product of a chemical reaction between ( i ) the photo - generated substance , and ( ii ) the dye precursor . this written form — the product of the chemical reaction that takes place only after photo activation — is a highly fluorescing dye . different generators and dye precursors were used to realize these novel memory materials . as one example , o - nitro - benzaldehyde was used as an acid generator . o - nitro - benzaldehyde undergoes phototransformation into a corresponding nitroso acid upon excitation with uv light . rhodamine b base was used as a dye precursor . rhodamine b base was found to react well with the photo induced nitroso - acid to form colored rhodamine b dye . after excitation with 355 nm light , the solution develops a strong pink color , and a bright red fluorescence was observed from this form when the solution was illuminated with 532 nm light . an identical color change and fluorescence were observed , after 355 nm irradiation when these same two components were dispersed in solid pmma matrices . in the case of solid matrices , both the unexposed and colored areas — i . e ., the unwritten and written areas — of the polymer film or block did not show any spectral changes or degradation at room , temperature , when they were stored in the dark . to increase the efficiency of the writing process yet another new memory material — 1 - nitro - 2 - naphthaldehyde ( nna )— was utilized as the acid generator component instead of o - nitro - benzaldehyde . it was found that , if excited with uv light , nna undergoes the same photochemical rearrangement to nitroso - acid as does o - nitro - benzaldehyde . the nitroso - acid , after excitation of nna with 355 nm light , reacts with rhodamine b base transforming this colorless dye precursor into a deeply colored fluorescing dye . accordingly , the initially colorless solution of the write form , composed of nna and rhodamine b base , is transformed to the colored , read form , when irradiated with uv light . the same process was observed when these components were dispersed in a rigid pmma matrix and excited with light of the same wavelength . this polymer based light sensitive molecular system was successfully used as a rom memory material . properties of the preferred chemical admixtures of the present invention may be approached through an understanding the photo rearrangement mechanism of 1 - nitro - 2 - naphthaldehyde and its application to 3d optical storage memory . the photo rearrangement of 1 - nitro - 2 - naphthaldehyde to the nitroso acid has been studied by the inventors through time - resolved picosecond and nanosecond spectroscopy . based on the experimental data contained in this specification , it is now postulated that the photo reaction proceeds via both the 1 nπ * excited singlet state and the low - lying 3 ππ * triplet state . photo . reactive 1 - nitro - 2 - naphthaldehyde is recognized to be suitable , along with a dye precursor and more particularly rhodamine dye precursor , as a new optical memory material . this material has been successfully demonstrated in two - photon three - dimensional ( 2 - p 3 - d .) optical storage devices . the photo isomerization of aromatic nitro compounds to nitroso compounds was reported initially by ciamician and silber . see ciamician , g . ; silber , p . ber . deutsch . chem . ges ., 34 ( 1901 ) 2040 . ciamician and silber observed that o - nitrobenzaldehyde was converted to o - nitrosobenzoic acid when exposed to sunlight . this process , was found to take place both in solution and in the crystalline state . since that time a number of other ortho - substituted nitro - aromatic compounds , which undergo similar photo rearrangement , have been studied . see schonberg , a . preparative organic photochemistry , springer - verlag new york , inc . : new york , 1968 ; pp 267 - 270 . in addition the o - nitrobenzaldehyde photo reaction has been used as an actinometer to measure solar uv radiation . see morales , r . g . e . ; jara , g . p . ; cabrera , s . limnol . oceanogr ., 38 ( 3 ) ( 1993 ) 703 . because of its importance as both a model for photo rearrangement and practical use , the mechanism of o - nitrobenzaldehyde phototransformation has been studied by several investigators in detail . see george , m . v . ; scaiano , j . c . j . phys . chem ., 84 ( 1980 ) 492 ; yip , r . w . ; sharma , d . k . res . chem . intermed ., 11 ( 1989 ) 109 ; kuberski , s . ; gebicki , j . j . molec . structure ,. 275 ( 1992 ) 105 ; mayo , p . ; reid , s . t . quart . rev ., 15 ( 1961 ) 393 ; yip , r . w . ; sharma , d . k . ; giasson , r . ; gravel , d . j . phys . chem ., 89 ( 1985 ) 5328 ; and schupp , h . ; wong , w . k . ; schnabel , w . j . photochem ., 36 ( 1987 ) 85 . it has been shown that the photo rearrangement of o - nitrobenzaldehyde proceeds via formation of a ketene intermediate . see george , et . al ., op cit . ; mayo , et al . op cit . ; yip ,. et al ., op cit . ; and schupp , et al ., op cit . decay into nitroso acid is accelerated by the presence of water . the ketene intermediate generated by uv excitation of matrix - isolated o - nitrobenzaldehyde was stabilized at low temperature ( 10 ° k ) and characterized by means of uv - vis . and ir spectroscopy . see kuberski , et . al ., op cit . the primary steps of the photo rearrangement of o - nitrobenzaldehyde into nitroso acid have been studied by means of time - resolved spectroscopy where some controversial data on the nature , of photo reactive excited electronic states were presented . see . george , et al ., op cit . ; and yip , et al . ( 1989 ), op cit . to the best knowledge of the inventors no direct experimental observations involving triplet or singlet excited states in the photochemical transformation of o - nitrobenzaldehyde have been reported . a study of the reaction mechanism of 1 - nitro - 2 - naphthaldehyde ( nna ), which undergoes an analogous photo rearrangement to nitroso acid , was undertaken . the following data , obtained by means of time - resolved picosecond and nanosecond spectroscopy and several analytic measurements , provides a rather complete understanding of the intermediates , final product , kinetics and mechanism of this photo reaction . from this understanding confidence in the radiative performance of an optical memory constructed from the chemicals , and in respect of the photo rearrangement reaction , may be had . based on photo reaction mechanism of nna , a novel photochromic material has been developed that has been spectroscopically qualified as useful for two - photon optical memories . this material has been - successfully utilized by the inventors for storing huge amounts of information inside a 3d volume and accessing the stored information in parallel , at a nanosecond transfer rate , by means of two photon absorption . see dvornikov , a . s . ; rentzepis , p . m . optics communications , 136 ( 1997 ) 1 . 1 - nitro - 2 - naphthaldehyde ( nna ) was synthesized according to the method described in makosza , m . ; owczarczyk , z . j . org . chem ., 54 ( 1989 ) 5094 . all starting chemicals were hplc purity and purchased from aldrich . the polymer materials were prepared by radical polymerization of methyl methacrylate solutions containing 10 − 1 m . nna , 10 − 4 m rhodamine b base and 2 × 10 − 2 m 2 , 2 ′- azobis ( 2 - methyl - propionitrile ) initiator . the polymerization process was carried out at 50 ° c . for ˜ 70 honors . the polymer blocks were cut to 1cm 3 cubes and polished to λ / 5 . the ground state absorption spectra were collected by a double beam shimadzu uv160u spectrophotometer , and the ir spectra were recorded by means of a nicolet 205 ft - ir spectrometer . nuclear magnetic resonance ( nmr ) spectra were recorded by means of a qe300 nmr spectrometer and mass spectra were recorded by means of vg analytical 7070e mass spectrometer . the picosecond transient absorption spectra and kinetics were measured by the laser system described by the inventors previously . see dvornikov , a . s . ; rentzepis , p . m ., res . chem . intermed ., 22 ( 1996 ) 115 . a single 35 ps , 355 nm third harmonic pulse , from a quantel nd : yag laser , was used for the excitation of nna solutions . the picosecond continuum used to detect the transient absorption spectra was generated by focusing the 532 nm or 1064 nm pulses into a cell containing the d 2 o / h 2 o mixture . the continuum pulse , after it passed through the volume of the sample cell , was analyzed by an oma system . changing the delay time between excitation and probe pulses permitted recording a complete histogram of the spectra of the transient species induced by the excitation pulse . the nanosecond kinetics and spectra of the transients were measured by an experimental system utilizing a continuum surlite ii nd : yag laser emitting 6 ns pulses at 1064 nm . the third harmonic , 355 nm , 3 mj pulse was used for excitation of the sample solutions . the probe beam , either a msec photoflash or a halogen projector lamp , was focused in the sample cell and then imaged , by a system of lenses , on the monochromator . the output slit of the monochromator was connected to a pmt ( hamamatsu r928 ) coupled to a digital tektronix tds 410a oscilloscope and computer . the same experimental system was used for both phosphorescence lifetime and transient spectra measurements in the nanosecond and longer time ranges . the 150 w xe arc lamp ( oriel research arc lamp source ) was used for continuous photochemical irradiation of the samples , using optical filters to select the appropriate wavelength . low temperature experiments were conducted in a four side quartz optical cell placed in a liquid nitrogen quartz dewar with , optical windows . the low temperature solvents used were 3 - methylpentane , methylcyclohexane and epa . the solutions were de - aerated by several freeze - pump - thaw cycles and sealed under vacuum . the method and experimental system for writing and reading information in 3d by means of two - photon absorption has been previously described in dvornikov , eta al . ( 1997 - 1 ), op , cit ,; and in dvornikov , a . s ., cokgor , i ., wang , m ., mccormick , f . b ., esener , s . e . and rentzepis , p . m . ieee cpmt - part a , 20 ( 1997 ) 203 . a . s . [ 10 , 13 ]. therefore this method and system will be presented , only briefly , in a later section . 2 . 3 results part 1 : spectroscopic properties and photo reaction quantum yield the absorption spectrum of nna is shown in fig1 . excitation of nna with uv light induced the formation of the yellow nitroso acid which has its absorption maximum at 395 nm , see fig1 . to verify that the final product of the photochemical reaction of nna is the nitroso acid , as is the case for o - nitrobenzaldehyde , the ir , nmr and mass spectra of this product were measured . a de - aerated concentrated solution of nna in cyclohexane was irradiated with uv light ( 150 w xe lamp , λ = 300 - 400 nm ) and the precipitated product of this photo reaction was is then collected , washed with solvent and dried . the ir spectrum of the product , fig2 was found to exhibit the characteristic absorption bands of carboxylic acids . the broad band at , 2800 cm − 1 is due to the o — h group , the sharp bands at 1700 cm − 1 and at 1250 cm − 1 are characteristic of the c ═ o and c — oh groups respectively . the 1 h — and 13 c — nmr spectra of the product exhibit characteristic peaks at δ 13 . 7 and at δ 167 respectively due to the presence of cooh in the molecule . similar peaks are observed for nitroso - acid , produced by photolisys of o - nitro - benzaldehyde . the mass spectrum shows the mass of the product is equal to 201 . 0426 , which is exact mass of 1 - nitroso - 2 - naphthalene carboxylic acid ( c 11 h 7 no 3 ). these data confirm , that the photo reaction of nna is a strictly intra molecular process of atom exchange between different molecular groups . it was found that photo rearrangement of nna to the nitroso acid is an irreversible process and no back photo reaction when nitroso acid is excited in its long wavelength absorption band with light λ & gt ; 400 nm was detected . prolonged irradiation of the nitroso acid , however , leads to photo decomposition of the molecules . because the nitroso acid is a relatively light stable compound , it was possible to measure its extinction coefficient rather accurately . the 10 − 4 m nna solution in acetonitrile was irradiated with uv light ( 150 w xe lamp , λ = 300 - 400 nm ) until no changes in the absorption spectra were observed . this implies that all of the nna is completely transformed into nitroso acid and that the concentration of the photo induced nitroso acid is equal to the initial concentration of nna . the extinction coefficient of the nitroso acid was calculated from the ratio of the absorbencies of nitroso acid and its precursor nna , see fig1 . the quantum yield of the phototransformation of nna into nitroso acid , which is the ratio of the number of nitroso acid molecules formed during the light excitation process to the number of photons absorbed by nna , was also measured . a 10 − 3 m de - aerated solutions of nna in different solvents ( see tab . 1 ) placed in a 1 cm quartz optical cell were irradiated with 355 nm light , emitted by the third harmonics of the surelite ii nd : yag laser . the excitation light energy was maintained at ˜ 7 mj / cm − 2 . at this energy level the dependence of the accumulation rate of nitroso acid vs energy was found to be linear , this eliminates the possibility of non - linear photo processes . the optical density of the solution at this wavelength is about 2 , therefore , practically all the light is absorbed by the solution . the light intensity was measured by means of aberchrome 540 chemical actinometer and also calculated using the , energy , measured by the molectron jd2000 joulemeter . see heller , h . g . ; langan , j . r . j . c . s . perkin . ii , ( 1981 ) 341 . both measurements showed the same result . the number of nitroso - acid molecules was calculated from its absorption spectrum and extinction coefficient , measured for specific solvent . the measurements were conducted under conditions where the accumulation of nitroso acid had a linear dependence on excitation time . the quantum yields are summarized in table 1 . the quantum yield is approximately 0 . 5 and does not depend on solvent polarity , however at 77 ° k ., the photochemical reaction of nna was found to occur with much lower quantum yield (˜ 0 . 04 ). when a solution of nna was irradiated with a 355 nm wavelength picosecond duration laser pulse , the formation of a transient species with the absorption spectrum shown in fig3 was observed . the rate of formation of this , the only intermediate observed in the kinetics experiments , was practically as fast as the excitation pulse duration , τ pulse ˜ 40 ps . fig4 shows a plot of the optical density change , of the long wavelength absorption maximum of the transient , vs . time . the accumulation rate constant value was measured to be 2 × 10 − 10 s − 1 . fig4 a a shows the evolution of the triplet state spectrum resulting from the intersystem crossing . at shorter lifetime , i . e . 25 ps , the spectra are composed of both s 1 → s n and t 1 → t n , while at later times , i . e . 75 ps , practically the whole spectrum is due to the triplet state alone . the decay of the transient followed first - order kinetics and the observed lifetime of the transient was found to increase with increasing solvent polarity . see table 2 . in fig1 . also , the absorption spectra of the transient species experienced a red shift in the long wavelength band , with solvent polarity , as shown in fig3 . this indicates that the transient has a considerable dipole . unlike o - nitrobenzaldehyde [ see george , et . al . ( 1080 ), op . cit . ], where the decay of the transient is strongly accelerated by the presence of water , no significant change in the transient kinetics when a small amount of water was added to solutions of nna was observed . instead , when a water / acetonitrile mixture was used as the solvent , the transient was found to be more stable . see table 2 in fig1 . in oxygen saturated solutions the decay rate of the transient is faster than in de - aerated solutions , as shown in fig5 . oxygen is more effective in polar solvents , where the lifetime of the transient is longer . in non - polar solvents , such as benzene , where the lifetime of the transient is about 50 ns , oxygen has practically no effect on the transient kinetics . this is expected because the reaction with oxygen is diffusion controlled . it should be noted that oxygen affects only the lifetime of the transient , while the intensity of the transient absorption remains the same in the presence and absence of oxygen . this is depicted in fig5 a , where the rate of decay with o 2 is shown to be faster than without o 2 . the quantum yield of the nitroso acid formation , measured by the transient absorption kinetics at 400 nm , where the nitroso acid has a strong absorption band , was found to decrease in the presence of oxygen , fig5 b . at 1 ms after excitation when the fast transient has practically no measurable absorption , only the non decaying absorption of the stable nitroso acid is observed . the decrease in optical density in the presence of oxygen corresponds therefore to a decrease in the photo reaction quantum yield . low temperature ( 77 ° k .) excitation of nna dispersed in epa and i - proh matrices induced high intensity phosphorescence which has the spectrum shown in fig6 a . the decay of the phosphorescence in epa matrix is shown in fig6 b , where the posphosphurescence intensity is plotted vs . time . the lifetime of the observed phosphorescence was estimated to be about 70 ms . the transient absorption spectra and kinetics after excitation of nna with a 355 nm laser pulse in glassy epa and i - proh matrices was measured at 77 ° k . the absorption spectrum of the transient , shown in fig7 a , is very similar to the one measured in liquid solutions at room temperature . the decay of this transient followed first - order kinetics with a lifetime of 65 ms , which is also the lifetime of the phosphorescence of nna in epa matrix at 77 ° k . the experimental data suggests that nna , like its close analog o - nitrobenzaldehyde , under light excitation undergoes photochemical rearrangement to the corresponding nitroso acid : the quantum yield of this transformation was found to be rather insensitive to the nature of the solvent and excitation light wavelength ( see table 1 in fig9 ), as has been observed for the photo reaction of o - nitrobenzaldehyde . see george , et al . ( 1980 ), op , cit . the lack of dependence of the reaction quantum yield on excitation light wavelength indicates that the photo reaction proceeds via the lowest electronic excited state . the reaction mechanism of o - nitrobenzaldehyde has been studied by several research groups [ e . g . george , et al . ( 1980 ), op , cit . ; and yip , et al . 91989 )., op . cit .] but no direct observations , which can prove the nature of the photoactive electronic excited state , were presented . because the photo reaction quantum yield was decreased [ see george et . al . ( 1980 ), op . cit .] by the addition of the triplet - state quencher , trans - 1 , 3 - pentadiene , it was suggested that the photo reaction of o - nitrobenzaldehyde proceeds via a short - lived triplet excited state . nevertheless , the authors of yip , et . al . ( 1989 ) ( op . cit . ), who studied the photo reaction of o - nitrobenzaldehyde by means of time - resolved spectroscopy , found no evidence of triplet excited states involved in the photochemical reaction , and instead suggested that the photo reaction proceeds via the photoactive singlet excited state . flash - photolysis studies of o - nitrobenzaldehyde detected the only intermediate that has been observed during its phototransformation into nitroso acid . this intermediate , assigned to a ketene structure , was found to be extremely sensitive to the presence of water due to catalysis of its transformation into nitroso acid . see george , et al . ( 1980 ), op cit . ; and yip , et al . ( 1989 ), op cit . the ketene intermediate in the photochemical reaction of o - nitrobenzaldehyde was also detected in matrix - isolation studies , at 10 k , by means of uv - vis and ir spectroscopy . see kuberski , s . ; as in the case of o - nitrobenzaldehyde , one intermediate was observed during photolysis of nna . its absorption spectra are shown in fig3 . unlike o - nitrobenzaldehyde , the lifetime of the intermediate formed during photolysis of nna was not affected by the presence of water but increased with increasing solvent polarity , as shown in table 2 of fig1 . these differences in the behavior of the intermediate observed , leads the inventors to suggest , that in the case of nna the reactive intermediate is a triplet excited state rather than the ketene intermediate , which was observed in the photolysis of o - nitrobenzaldehyde . as it can be expected for nitro - and formyl - substituted naphthalenes , excitation of nna at 355 nm results in the population of the 1 nπ * state , ( ε ≈ 2200 ). see calvert , j . g . ; pitts , j . n . photochemistry , wiley , n . y ., 1966 , p . 369 ; turro , n . j . molecular photochemistry , w . a . benjamin , n . y ., 1967 p . 15 ; jaffe , h . h . ; orchin m . theory and applications of ultraviolet spectroscopy , wiley , n . y ., 1962 , p . 213 ; itih , i . spectrochimica acta part a , 52 ( 1996 ) 343 ; yagi , m . ; shioya , y . ; higuchi , j . j . photochem . photobiol . a :, 62 ( 1991 ) 65 ; and martins , l . ; fernandes , m . ; kemp , t . ; formosinho , s . ; branco , j . j . chem . soc . faradey trans ., 87 ( 1991 ) 3617 . the absorption maximum of this band was found to have a red shift from 345 nm in polar acetonitrile to 348 nm in non - polar cyclohexane solutions , suggesting 1 nπ * character for this state . there are also two ππ * states in the uv area of 230 nm to 300 nm with ε 245 = 42 , 100 and ε 287 = 7 , 400 . the excited nπ * state relaxes with a lifetime of 50 ps ( fig4 ) to a lower lying excited state which is assigned to a triplet state , 3 ππ * based on the data presented above . the intersystem crossing rate of 2 × 10 10 s − 1 is commensurate with an 1 nπ * initial level decaying into a 3 ππ * triplet state . this fast rate is responsible for a highly populated triplet state and consequently for the strong t 1 → t n absorption observed with a maximum at ˜ 580 nm . the location of the charge transfer bands play a dominant role in the isc rate . in the case of nna the ct band is expected to be in the higher energy region , as is in 1 - nitronaphthalene ( e . g . 8 . 5 ev [ 21 ]), but contribute to the 3 ππ * character . this ct contribution again favors a fast 1 nπ *→ 3 ππ * rate . the measured 50 ps triplet formation time constant is slower than the 13 ps time constant observed for 1 - nitronaphthalene because of the larger separation of the states involved in nna . a further support to the 3 ππ * assignment of the transient is the red shift which was observed of its long wavelength absorption band with increasing solvent polarity . from the phosphorescence spectrum , fig6 a , the location of the transient 0 - 0 band absorption was found to be 510 nm ( 19 , 600 cm − 1 ) where the 1 - nitronaphthalene ct , 3 ππ * band is also located . see ohtani , h ; kobayashi , t ; suzuki , k ; nagakura , s . bull . chem . soc . jpn ., 53 ( 1980 ) 43 . this provides further support for the 3 ππ * assignment of the transient . assignment to a 3 nπ * is not favored because of the large st separation of ˜ 18 , 000 cm − 1 ( 50 kcal ) and the red shift observed with solvent polarity . stabilization of this triplet state by polar solvents suggests a considerable increase in the dipole moment of the triplet state . in polar solvents , such as acetonitrile and alcohols , where the lifetime of the observed triplet state is about 200 - 300 ns ( see table 2 in fig1 ) it was found that oxygen accelerates its decay rate , while the intensity of the signal due to - triplet - triplet absorption at zero - time ( right after the excitation with a 6 ns laser pulse ) remains the same . see fig5 . the decay rate constant of the triplet state in the presence of a triplet quencher , such as oxygen , may be represented as : k = ko + k q [ o 2 ], where k o is the rate constant in the absence of oxygen ; k q is the quenching constant and [ o 2 ] is the concentration of oxygen . in de - aerated and oxygen saturated acetonitrile solutions the decay rate constants were measured and found to be equal to 3 . 1 × 10 6 and 2 × 10 7 m − 1 s − 1 respectively . the concentration of oxygen in oxygen saturated solution is about 9 . 5 × 10 - 3 m 15 . from these data the triplet quenching constant was estimated to be k q ˜ 1 . 8 × 10 9 m − 1 s − 1 . this value corresponds to the triplet quenching by oxygen . see murov , s . l . handbook of photochemistry , marcel dekker , inc . : new york , 1973 ; p . 59 , 89 . to further establish that the observed intermediate is the excited triplet state of nna , experiments were conducted at 77 ° k ., in epa and i - proh matrices . the bright phosphorescence of the excited nna molecules , dispersed in solid matrices at 77 ° k ,. was observed in the region of 520 - 580 nm , and is shown in fig6 a . the triplet - triplet absorption spectrum , measured at 77 ° k . ( see fig7 a ), is found to be the same as the spectrum measured at room temperature . this fact suggests that the same intermediate is observed at both temperatures . the decay rate of the triplet state at 77 ° k , measured by the decrease of the triplet - triplet absorption intensity as a function of time , also corresponds to the phosphorescence decay rate , see fig6 b and 7 b . the quantum , efficiency of the photochemical reaction at 77 ° k . decreases by an be order of magnitude compared to the one measured at room temperature . these data are listed in table 1 of fig9 . it should be noted that in non - polar matrices at 77 ° k ., such as 3 - methylpentane and methylcyclohexane , only weak phosphorescence was observed and the quantum efficiency of the photo process was found to be higher than in polar matrices . these data are also presented in table 1 of fig9 . the quenching of the photochemically active triplet state by oxygen leads to a decrease in the photo reaction quantum yield , observed in polar solvents , see fig5 . in non - polar solvents , where the decay time of the triplet state is shorter than 50 ns , the effect of oxygen was not observed , because at that rate the concentration of oxygen was not enough to quench the triplet state . fig5 b shows that in oxygen saturated acetonitrile solutions the photo reaction quantum yield was found to be 1 . 4 times less than the quantum yield in de - aerated solutions . the lifetime of the triplet excited state was found to decrease by a factor of 4 . 6 under the same conditions , these data are shown in fig5 a . when the product of the photo reaction is formed exclusively via the triplet excited state , then the quenching of this photoactive electronic excited state should also result in the decrease of the photo reaction quantum yield . the difference in the decrease of nitroso acid quantum yield and triplet excited state lifetime found in our experiments suggests that part of the product is formed via the singlet excited state . the total quantum yield of the photo reaction was measured to be 0 . 5 , see table 1 . this suggest that an internal conversion deactivation process of the singlet excited state competes effectively with singlet to triplet intersystem crossing and the photo reaction . this is substantiated by the fact that no fluorescence was detected in nna solutions . the formation rate constant of the triplet excited state which corresponds to the decay constant of the singlet excited state , was measured to be 2 × 10 10 sec − 1 ( see . fig4 ). these results prompt the inventors to propose the following reaction scheme , quantum efficiencies and rate constants for the processes involved in the phototransformation of nna : the ketene intermediate was not observed during photolysis of nna , but the involvement of this product is suggested by analogy with the photo reaction of o - nitrobenzaldehyde , where the ketene transient was detected . the inventor &# 39 ; s failure to observe the ketene intermediate in the case of nna may be due to its relatively low absorption intensity compared to the observed triplet - triplet absorption . the absorption spectra of the ketene and the triplet state are expected to overlap and consequently the ketene absorption spectrum may be masked . 3 . use of the preferred chemicals as 2 - p 3 - d optical memory materials the two forms of the molecule represent the 0 and 1 of the computer binary code . the original form , non irradiated form , corresponds to the zero of the binary code . when this molecule is excited it undergoes a photochemical transformation to a colored form corresponding to the binary code 1 . the forms corresponding to 0 and 1 in the binary code may be either ( i ) reversible , whereupon they form a write / read / erase memory or ( ii ) so that the back reaction is not possible , resulting in a write once read many , or worm , memory . selection of voxels within a 3d volume is achieved by means of two photon absorption process previously described by the inventors , and the subject of a patent of one inventor . see dvornikov , a . s . ; rentzepis , p . m . optics communications , 136 ( 1997 ). briefly , two pulsed beams intersect each other inside the bulk of the device as shown schematically in fig8 a . neither beam has enough energy — i . e ., the wavelength is too long — to , individually excite the molecule to an excited state . however , when the two beams intersect then their combined energies are sufficient to populate the first excited state . this is shown by means of an energy level diagram in fig8 b . subsequent photochemistry transforms the original molecule to the “ written ” form corresponding to a “ 1 ” in the binary code . the information is accessed by exciting the “ written ” form to its first excited singlet state and recording its fluorescence by means of a ccd . subsequently the information is digitized and processed as the information from a magnetic disk . in addition to the fact that a huge amount of information may be stored , i . e ., 10 12 b / cm 3 , the information can be stored and accessed in parallel , i . e . a complete 100 mb disk may be stored and accessed simultaneously , rather than by the normal bit - by - bit process . the 3d memory based on nna is by design a worm device , where information can be written once only but can be accessed many times . the process of making a memory device consists of dispersing nitro - naphthaldehyde and rhodamine b base within a matrix in the form of , most typically , a cube ( of , for example , 1 cm 3 ) or a thick disk ( of , for example , a 8 cm ( 3 ″) diameter by a 1 . 25 cm ( ½ ″) thickness ). the rhodamine b base corresponds to the “ write ” form , “ 0 ” in the binary code . the cube or disk is irradiated with 532 nm and 1064 nm ps laser pulses shaped into 8 mm 2 × 20 μm thick plane beam . the 1064 nm information beam passes through an slm ( spatial light modulator ) which contains the information to be stored , and propagates through the cube . the 532 nm , reference , beam propagates also into the cube following an optical path perpendicular to the information beam . where the two beams intersect light is absorbed , nna generates nitroso acid , and photochemistry induces the rhodamine b base to become rhodamine b which is the “ read ” form corresponding to 1 in the binary code : rhodamine b when excited fluoresces very strongly . more precisely , its quantum efficiency is approximately 1 . therefore it is very well suited for accessing information . reading is achieved by exciting a page with a 532 nm plane beam and recording the rhodamine b fluorescence . using these materials and the two photon method described here briefly , the inventors and their collaborators have been able to store in the bulk of a 1 cm 3 cube more than one hundred 2 d disks ( pages ) each containing 10 mb / disk of information . see dvornikov , a . s . ; rentzepis , p . m ., optics communications , 136 ( 1997 ); dvornikov , a . s . ; rentzepis , p . m ., res . chem . intermed ., 22 ( 1996 ) 115 ; and dvornikov , a . s ., cokgor , i ., wang , m ., mccormick , f . b ., esener , s . e . and rentzepis , p . m ., ieee - cpmt — part a , 20 , ( 1997 ) 203 . the chemical and radiation responses of the constituent chemicals and photochemicals of the present invention are summarized in fig1 a through 11 e . fig1 a shows the phtoisomerization of aromic nitro compounds to nitroso compounds , as previously reported in the literature . fig1 b shows the phototransformation of nna into a corresponding nitroso acid . fig1 c shows the photoreaction of intermediate product o - nitrobenzaldehyde in the presence of water . fig1 d shows the photolysis of nna . fig1 e shows the chemical transformation of dye precursor rhodamine b base into dye rhodamine b in the presence of nitroso acid . still other acid generators and chemical amplifiers are suitable . for example , onium salts such as triphenylsulfonium tetrafluroborate and diphenyliodonium tetrafluoroborate are suitable . the - phototransformation of nna into nitroso acid is shown to proceed via both singlet 1 nπ * and triplet 3 ππ * excited states . the quantum yield is rather insensitive to the polarity of the solvent and excitation light wavelength . the lifetime of the 3 ππ * triplet state was found to increase with increasing solvent polarity and in highly polar solvents was long enough to allow the triplet state to be quenched by oxygen . the decrease of the photo reaction quantum yield in the presence of oxygen was also measured . at low temperatures , . i . e ., 77 ° k ., the photo reaction of nna was found to proceed with considerably lower quantum yield , while a bright phosphorescence was detected and found to be the dominant deactivation channel of the triplet excited state . based on experimental data and literature data available , a mechanism for the phototransformation of 1 - nitro - 2 - naphthaldehyde into nitroso acid is proposed . this material forms the basis for a novel 3d storage computer memory device . nna has been utilized as an acid generator in photochromic memory material , composed of nna and rhodamine b base dispersed in a pmma host . the application of this new memory material to optical memory stores , and , particularly , to 3d optical storage devices with such memory stores , has been demonstrated . in accordance with the preceding explanation , variations and adaptations of the chemical and photochemical admixtures , and the optical memory stores realizable with these admixtures , in accordance with the present invention will suggest themselves to a practitioner of the chemical , photochemical and / or optical / radiation memory arts . for example , once the concept of changing a first , photosensitive , chemical so as to react with a second , dye precursor , chemical in order to form a stable dye is understood , than it is a straightforward matter to search , first , for ( i ) any dye that can be made by combination with any of acids , bases , ions , radicals and / or excited molecules from some dye precursor and then , second , for ( ii ) some means of photochemically making — possibly in more than one reaction step — the acids , bases , ions or radicals , and / or excited molecules with which the dye precursor is reactive . for example , the phototransformation step can be indirect . consider activation by light of a molecule that subsequently transfers its energy ( as was received by the light radiation ) to yet another , “ next ”, molecule . this “ next ” molecule then undergoes phototransformation to another form , which other form is reactive with the dye precursor molecule to form the dye . for example , and as already tangentially mentioned , the written form of the chemical can be either the fluorescing ( as is the preferred embodiment taught herein ), or , alternatively , the non - fluorescing , of two complimentary forms . in each case , the initial , un - written , form — whether fluorescing or not — is normally designated as binary “ 0 ” while the opposite , written , form is designated as binary “ 1 ”. for example , it may be contemplated that other sets of ( i ) dye precursor and ( ii ) generator molecules could be found , and used , so as to , when radiatively stimulated , chemically react together to generate a material that would and could subsequently be radiatively stimulated to fluoresce . however , and as a more radical extension of the present invention , the “ end item ” to be sought might not be flourescence , but electrical conductivity in a sort of optically - stimulated electrically - interrogated memory . in this case a set of ( i ) precursor molecules to the creation of an electrically conductive molecules and ( ii ) generator molecules responsive to radiation for producing something — an acid , perhaps for changing the precursor molecules into their electrically conductive state , would be sought , and used . in other words , this chemical / photochemical pair would , when radiatively stimulated , chemically react together to generate a material that would , when subsequently radiatively stimulated , exhibit discernable electrical — and not ( necessarily ) optical — properties . it will thus be recognized that the present invention spans many photochemical , and chemical , combinations that are within the spirit of the invention for stably inducing a radiation - detectable ( i . e ., readable ) change in some first molecules within a domain , or voxel , in response to the radiation - induced phototransformation of second molecules co - occupying the same domain ( i . e ., writing ). in accordance with these and other possible variations and adaptations of the present invention , the scope of the invention should be determined in accordance with the following claims , only , and not solely in accordance with that embodiment within which the invention has been taught .