《量子力学》The wave nature of the electron

LOUIS DE BROGLIE The wave nature of the electron Nobel Lecture. December 12. 1929 When in 1920 I resumed my studies of theoretical physics which had long been interrupted by circumstances beyond my control, I was far from the idea that my studies would bring me several years later to receive such a higl and envied prize as that awarded by the Swedish Academy of Sciences each year to a scientist: the Nobel Prize for Physics. What at that time drew me towards theoretical physics was not the hope that such a high distinction would ever crown my work; I was attracted to theoretical physics by the mystery enshrouding the structure of matter and the structure of radiations, a mystery which deepened as the strange quantum concept introduced by Planck in 1900 in his research on black-body radiation continued to encroach on the whole domain of physics To assist you to understand how my studies developed, I must first depict for you the crisis which physics had then been passing through for some twenty years For a long time physicists had been wondering whether light was composed of small, rapidly moving corpuscles. This idea was put forward by the phi- losophers of antiquity and upheld by Newton in the 18th century. After Thomas Young s discovery of interference phenomena and following the admirable work of Augustin Fresnel, the hypothesis of a granular structure of light was entirely abandoned and the wave theory unanimously adopted Thus the physicists of last century spurned absolutely the idea of an atomic structure of light. Although rejected by optics, the atomic theories began making great head way not only in chemistry, where they provided a simple interpretation of the laws of definite proportions, but also in the physics of matter where they made possible an interpretation of a large number of prop- erties of solids, liquids, and gases. In particular they were instrumental in the elaboration of that admirable kinetic theory of gases which, generalized un- der the name of statistical mechanics, enables a clear meaning to be given to the abstract concepts of thermodynamics. Experiment also yielded decisive proof in favour of an atomic constitution of electricity; the concept of the

L OUIS DE B ROGLI E The wave nature of the electron Nobel Lecture, December 12, 1929 When in 1920 I resumed my studies of theoretical physics which had long been interrupted by circumstances beyond my control, I was far from the idea that my studies would bring me several years later to receive such a high and envied prize as that awarded by the Swedish Academy of Sciences each year to a scientist: the Nobel Prize for Physics. What at that time drew me towards theoretical physics was not the hope that such a high distinction would ever crown my work; I was attracted to theoretical physics by the mystery enshrouding the structure of matter and the structure of radiations, a mystery which deepened as the strange quantum concept introduced by Planck in 1900 in his research on black-body radiation continued to encroach on the whole domain of physics. To assist you to understand how my studies developed, I must first depict for you the crisis which physics had then been passing through for some twenty years. For a long time physicists had been wondering whether light was composed of small, rapidly moving corpuscles. This idea was put forward by the phi￾losophers of antiquity and upheld by Newton in the 18th century. After Thomas Young’s discovery of interference phenomena and following the admirable work of Augustin Fresnel, the hypothesis of a granular structure of light was entirely abandoned and the wave theory unanimously adopted. Thus the physicists of last century spurned absolutely the idea of an atomic structure of light. Although rejected by optics, the atomic theories began making great headway not only in chemistry, where they provided a simple interpretation of the laws of definite proportions, but also in the physics of matter where they made possible an interpretation of a large number of prop￾erties of solids, liquids, and gases. In particular they were instrumental in the elaboration of that admirable kinetic theory of gases which, generalized un￾der the name of statistical mechanics, enables a clear meaning to be given to the abstract concepts of thermodynamics. Experiment also yielded decisive proof in favour of an atomic constitution of electricity; the concept of the

WAVE NATURE OF ELECTRON 245 electricity corpuscle owes its appearance to Sir J. J. Thomson and you will all be familiar with H. A. Lorentz, s use of it in his theory of electrons Some thirty years ago, physics was hence divided into two: firstly the physics of matter based on the concept of corpuscles and atoms which were supposed to obey Newtons classical laws of mechanics, and secondly radia- tion physics based on the concept of wave propagation in a hypothetical continuous medium, i.e. the light ether or electromagnetic ether. But these two physics could not remain alien one to the other; they had to be fused together by devising a theory to explain the energy exchanges between mat ter and radiation-and that is where the difficulties arose. While seeking to link these two physics together, imprecise and even inadmissible conclu- sions were in fact arrived at in respect of the energy equilibrium between matter and radiation in a thermally insulated medium: matter, it came to be said, must yield all its energy to the radiation and so tend of its own accord to absolute zero temperature! This absurd conclusion had at all costs to be avoided. By an intuition of his genius Planck realized the way of avoiding it: instead of assuming, in common with the classical wave theory, that light source emits its radiation continuously, it had to be assumed on the contrary that it emits equal and finite quantities, quanta. The energy of each quantum has, moreover, a value proportional to the frequency u of the ra- diation. It is equal to h, h being a universal constant since referred to as Plancks constant The success of Planck's ideas entailed serious consequences. If light is emit- ted as quanta, ought it not, once emitted, to have a granular structure? The existence of radiation quanta thus implies the corpuscular concept of light On the other hand, as shown by Jeans and H. Poincare, it is demonstrable that if the motion of the material particles in light sources obeyed the laws of classical mechanics it would be impossible to derive the exact law of black body radiation, Plancks law. It must therefore be assumed that traditiona dynamics, even as modified by Einstein s theory of relativity, is incapable of accounting for motion on a very small scale The existence of a granular structure of light and of other radiations was confirmed by the discovery of the photoelectric effect. If a beam of light or of X-rays falls on a piece of matter, the latter will emit rapidly moving elec trons. The kinetic energy of these electrons increases linearly with the fre- quency of the incident radiation and is independent of its intensity. This phenomenon can be explained simply by assuming that the radiation is com- posed of quanta lo capable of yielding all their energy to an electron of the

WAVE NATURE OF ELECTRON 245 electricity corpuscle owes its appearance to Sir J. J. Thomson and you will all be familiar with H. A. Lorentz’s use of it in his theory of electrons. Some thirty years ago, physics was hence divided into two: firstly the physics of matter based on the concept of corpuscles and atoms which were supposed to obey Newton’s classical laws of mechanics, and secondly radia￾tion physics based on the concept of wave propagation in a hypothetical continuous medium, i.e. the light ether or electromagnetic ether. But these two physics could not remain alien one to the other; they had to be fused together by devising a theory to explain the energy exchanges between mat￾ter and radiation - and that is where the difficulties arose. While seeking to link these two physics together, imprecise and even inadmissible conclu￾sions were in fact arrived at in respect of the energy equilibrium between matter and radiation in a thermally insulated medium: matter, it came to be said, must yield all its energy to the radiation and so tend of its own accord to absolute zero temperature! This absurd conclusion had at all costs to be avoided. By an intuition of his genius Planck realized the way of avoiding it: instead of assuming, in common with the classical wave theory, that a light source emits its radiation continuously, it had to be assumed on the contrary that it emits equal and finite quantities, quanta. The energy of each quantum has, moreover, a value proportional to the frequency v of the ra￾diation. It is equal to hv, h being a universal constant since referred to as Planck’s constant. The success of Planck’s ideas entailed serious consequences. If light is emit￾ted as quanta, ought it not, once emitted, to have a granular structure? The existence of radiation quanta thus implies the corpuscular concept of light. On the other hand, as shown by Jeans and H. Poincaré, it is demonstrable that if the motion of the material particles in light sources obeyed the laws of classical mechanics it would be impossible to derive the exact law of black￾body radiation, Planck’s law. It must therefore be assumed that traditional dynamics, even as modified by Einstein’s theory of relativity, is incapable of accounting for motion on a very small scale. The existence of a granular structure of light and of other radiations was confirmed by the discovery of the photoelectric effect. If a beam of light or of X-rays falls on a piece of matter, the latter will emit rapidly moving elec￾trons. The kinetic energy of these electrons increases linearly with the fre￾quency of the incident radiation and is independent of its intensity. This phenomenon can be explained simply by assuming that the radiation is com￾posed of quanta hv capable of yielding all their energy to an electron of the

1929 L DE BROGLIE irradiated body: one is thus led to the theory of light quanta proposed Einstein in 1905 and which is, after all, a reversion to Newtons corpuscular theory, completed by the relation for the proportionality between the en- ergy of the corpuscles and the frequency. A number of arguments were put forward by Einstein in support of his viewpoint and in 1922 the discovery by A H. Compton of the X-ray scattering phenomenon which bears his name confirmed it. Nevertheless, it was still necessary to adopt the wave theory to account for interference and diffraction phenomena and no way whatsoever of reconciling the wave theory with the existence of light cor- puscles could be visualized As stated, Planck's investigations cast doubts on the validity of very small scale mechanics. Let us consider a material point which describes a small tra- jectory which is closed or else turning back on itself. According to classical dynamics there are numberless motions of this type which are possible com- plying with the initial conditions, and the possible values for the energy of the moving body form a continuous sequence On the other hand Planck was led to assume that only certain preferred motions, quantized motions, are possible or at least stable, since energy can only assume values forming a discontinuous sequence. This concept seemed rather strange at first but its value had to be recognized because it was this concept which brought Planck to the correct law of black-body radiation and because it then proved its uitfulness in many other fields. Lastly, it was on the concept of atomic mo- tion quantization that Bohr based his famous theory of the atom; it is so familiar to scientists that i shall not summarize it here The necessity of assuming for light two contradictory theories-that of waves and that of corpuscles-and the inability to understand why, among the infinity of motions which an electron ought to be able to have in the atom according to classical concepts, only certain ones were possible: such were the enigmas confronting physicists at the time I resumed my studies of When I started to ponder these difficulties two things struck me in the main. Firstly the light-quantum theory cannot be regarded as satisfactory since it defines the energy of a light corpuscle by the relation W= hu which con- ains a frequency D. Now a purely corpuscular theory does not contain any element permitting the definition of a frequency. This reason alone renders it necessary in the case of light to introduce simultaneously the corpuscle concept and the concept of periodicity

246 1929 L.DE BROGLIE irradiated body: one is thus led to the theory of light quanta proposed by Einstein in 1905 and which is, after all, a reversion to Newton’s corpuscular theory, completed by the relation for the proportionality between the en￾ergy of the corpuscles and the frequency. A number of arguments were put forward by Einstein in support of his viewpoint and in 1922 the discovery by A. H. Compton of the X-ray scattering phenomenon which bears his name confirmed it. Nevertheless, it was still necessary to adopt the wave theory to account for interference and diffraction phenomena and no way whatsoever of reconciling the wave theory with the existence of light cor￾puscles could be visualized. As stated, Planck’s investigations cast doubts on the validity of very small scale mechanics. Let us consider a material point which describes a small tra￾jectory which is closed or else turning back on itself. According to classical dynamics there are numberless motions of this type which are possible com￾plying with the initial conditions, and the possible values for the energy of the moving body form a continuous sequence. On the other hand Planck was led to assume that only certain preferred motions, quantized motions, are possible or at least stable, since energy can only assume values forming a discontinuous sequence. This concept seemed rather strange at first but its value had to be recognized because it was this concept which brought Planck to the correct law of black-body radiation and because it then proved its fruitfulness in many other fields. Lastly, it was on the concept of atomic mo￾tion quantization that Bohr based his famous theory of the atom; it is SO familiar to scientists that I shall not summarize it here. The necessity of assuming for light two contradictory theories-that of waves and that of corpuscles - and the inability to understand why, among the infinity of motions which an electron ought to be able to have in the atom according to classical concepts, only certain ones were possible: such were the enigmas confronting physicists at the time I resumed my studies of theoretical physics. When I started to ponder these difficulties two things struck me in the main. Firstly the light-quantum theory cannot be regarded as satisfactory since it defines the energy of a light corpuscle by the relation W = hv which con￾tains a frequency v. Now a purely corpuscular theory does not contain any element permitting the definition of a frequency. This reason alone renders it necessary in the case of light to introduce simultaneously the corpuscle concept and the concept of periodicity

WAVE NATURE OF ELECTRON 247 On the other hand the determination of the stable motions of the electrons in the atom involves whole numbers, and so far the only phenomena in which whole numbers were involved physics were ose of interference selves could not be represented as simple corpuscles either, but that a Pen and of eigenvibration. That suggested the idea to me that electrons then odicity had also to be assigned to them too. thus arrived at the following overall concept which guided my studies for both matter and radiations, light in particular, it is necessary to introduce the corpuscle concept and the wave concept at the same time. In other words the existence of corpuscles accompanied by waves has to be assumed in all according to Bohrs expression, they constitute two complementary forces of reality, it must be possible to establish a certain parallelism between the motion of a corpuscle and the propagation of the associated wave. The first objective to achieve had, therefore, to be to establish this correspondence. With that in view I started by considering the simplest case: that of an isolated corpuscle, i.e. a corpuscle free from all outside influence. We wish to associate a wave with it. Let us consider first of all a reference syster oxoyozo in which the corpuscle is immobile: this is the intrinsic" system of the corpuscle in the sense of the relativity theory. In this system the wave will be stationary since the corpuscle is immobile: its phase will be the same at every point; it will be represented by an expression of the form sin 2Zvol(to-To); to being the intrinsic time of the corpuscle and to a constant. In accordance with the principle of inertia in every Galilean system, the orpuscle will have a rectilinear and uniform motion. Let us consider such Galilean system and let v=Bc be the velocity of the corpuscle in this system; we shall not restrict generality by taking the direction of the motion as the x-axis. In compliance with Lorentz' transformation, the time t used by an observer of this new system will be associated with the intrinsic time to by the relation -B2 and hence for this observer the phase of the wave will be given by √1-B( Bx

WAVE NATURE OF ELECTRON 247 On the other hand the determination of the stable motions of the electrons in the atom involves whole numbers, and so far the only phenomena in which whole numbers were involved in physics were those of interference and of eigenvibrations. That suggested the idea to me that electrons them￾selves could not be represented as simple corpuscles either, but that a peri￾odicity had also to be assigned to them too. I thus arrived at the following overall concept which guided my studies: for both matter and radiations, light in particular, it is necessary to introduce the corpuscle concept and the wave concept at the same time. In other words the existence of corpuscles accompanied by waves has to be assumed in all cases. However, since corpuscles and waves cannot be independent because, according to Bohr’s expression, they constitute two complementary forces of reality, it must be possible to establish a certain parallelism between the motion of a corpuscle and the propagation of the associated wave. The first objective to achieve had, therefore, to be to establish this correspondence. With that in view I started by considering the simplest case: that of an isolated corpuscle, i.e. a corpuscle free from all outside influence. We wish to associate a wave with it. Let us consider first of all a reference system o~~y~z~ in which the corpuscle is immobile: this is the "intrinsic" system of the corpuscle in the sense of the relativity theory. In this system the wave will be stationary since the corpuscle is immobile: its phase will be the same at every point; it will be represented by an expression of the form sin ZZV~(~~~~) ; to being the intrinsic time of the corpuscle and to a constant. In accordance with the principle of inertia in every Galilean system, the corpuscle will have a rectilinear and uniform motion. Let us consider such a Galilean system and let t, = ,dc be the velocity of the corpuscle in this system; we shall not restrict generality by taking the direction of the motion as the x-axis. In compliance with Lorentz’ transformation, the time t used by an observer of this new system will be associated with the intrinsic time to by the relation: and hence for this observer the phase of the wave will be given by

1929 L DE BROGLIE For him the wave will thus have a frequency: √r-B2 and will propagate in the direction of the x-axis at the phase velocity: By the elimination of B between the two preceding formulae the following elation can readily be derived which defines the refractive index of the vacuum n for the waves considered A > corresponds to this >. You will be aware that the group velocity is the velocity of the resultant amplitude of a group of waves of very close frequencies. Lord Rayleigh showed that this velocity u satisfies equation I a(nm) Here U=v, that is to say that the group velocity of the waves in the system ryxt is equal to the velocity of the corpuscle in this system. This relation is of very great importance for the development of the theory The corpuscle is thus defined in the system ryzt by the frequenc e phase velocity V of its associated wave. To establish the parallelism of which we have spoken, we must seek to link these parameters to the me. chanical parameters, energy and quantity of motion. Since the proportion- ality between energy and frequency is one of the most characteristic relations of the quantum theory, and since, moreover, the frequency and the energy transform in the same way when the Galilean reference system is changed, we may simply write nergy=h x frequency, or W=hu

248 1929 L.DE BROGLI E For him the wave will thus have a frequency: and will propagate in the direction of the x-axis at the phase velocity: By the elimination of b between the two preceding formulae the following relation can readily be derived which defines the refractive index of the vacuum n for the waves considered: J 2 fi-= p2- V2 A > corresponds to this >. You will be aware that the group velocity is the velocity of the resultant amplitude of a group of waves of very close frequencies. Lord Rayleigh showed that this velocity U satisfies equation : I -=-- a (4 U &J Here U = v, that is to say that the group velocity of the waves in the system xyxt is equal to the velocity of the corpuscle in this system. This relation is of very great importance for the development of the theory. The corpuscle is thus defined in the system xyzt by the frequency v and the phase velocity V of its associated wave. To establish the parallelism of which we have spoken, we must seek to link these parameters to the me￾chanical parameters, energy and quantity of motion. Since the proportion￾ality between energy and frequency is one of the most characteristic relations of the quantum theory, and since, moreover, the frequency and the energy transform in the same way when the Galilean reference system is changed, we may simply write energy = h x frequency, or W = h v

WAVE NATURE OF ELECTRON 249 where h is Planck's constant. This relation must apply in all Galilean systems and in the intrinsic system of the corpuscle where the energy of the corpuscle, according to Einstein, reduces to its internal energy mc(m being the rest mass we have Inoo= nm This relation defines the frequency voas a function of the rest mass m, or The quantity of movement is a vector p equal to mov and we have The quantity; n is the distance between two consecutive peaks of the wave, This is a fundamental relation of the theory The whole of the foregoing relates to the very simple case where there is no field of force at all acting on the corpuscles. I shall show you very briefly how to generalize the theory in the case of a corpuscle moving in a constant field of force deriving from a potential function F(xyz). By reasoning which I shall pass over, we are then led to assume that the propagation of the wave corresponds to a refractive index which varies from point to point in space in accordance with the formula )--

WAVE NATURE OF ELECTRON 249 where h is Planck’s constant. This relation must apply in all Galilean systems and in the intrinsic system of the corpuscle where the energy of the corpuscle, according to Einstein, reduces to its internal energy moc 2 (m0 being the rest mass) we have hvo = moc 2 This relation defines the frequency vO as a function of the rest mass mo , or inversely. The quantity of movement is a vector p equal to and we have: (p)= lfbv -WV hv-h 2/I=2- c2 =-F-n The quantity; l is the distance between two consecutive peaks of the wave, i.e. the "wavelength". Hence: This is a fundamental relation of the theory. The whole of the foregoing relates to the very simple case where there is no field of force at all acting on the corpuscles. I shall show you very briefly how to generalize the theory in the case of a corpuscle moving in a constant field of force deriving from a potential function F(xyz). By reasoning which I shall pass over, we are then led to assume that the propagation of the wave corresponds to a refractive index which varies from point to point in space in accordance with the formula:

1929 L. DE BROGLIE or to a first approximation if the corrections introduced by the theory of relativity are negligible ith E=w- moc The constant energy w of the corpuscle is still as- sociated with the constant frequency y of the wave by the relation while the wavelength a which varies from one point to another of the force field is associated with the equally variable quantity of motion p by the fol- lowing relation x2)=p(xy2) lere again it is demonstrated that the group velocity of the waves is equal to the velocity of the corpuscle. The parallelism thus established between the orpuscle and its wave enables us to identify Fermat's principle for the waves and the principle of least action for the corpuscles(constant fields). Fermat's principle states that the ray in the optical sense which passes through two points A and B in a medium having an index n(xyz)varying from one point to another but constant in time is such that the integral aken along this ray is extreme. On the other hand Maupertuis principle least action teaches us the following: the trajectory of a corpuscle passi through two points A and B in space is such that the integral p taken along the trajectory is extreme, provided, of course, that only the motions corresponding to a given energy value are considered. From the relations derived above between the mechanical and the wave parameters, we have C I h hz一P const

250 1929 L. DE BROGLIE or to a first approximation if the corrections introduced by the theory of relativity are negligible with E = W - m0c2. The constant energy W of the corpuscle is still as￾sociated with the constant frequency Y of the wave by the relation while the wavelength 1 which varies from one point to another of the force field is associated with the equally variable quantity of motion p by the fol￾lowing relation Here again it is demonstrated that the group velocity of the waves is equal to the velocity of the corpuscle. The parallelism thus established between the corpuscle and its wave enables us to identify Fermat’s principle for the waves and the principle of least action for the corpuscles (constant fields). Fermat’s principle states that the ray in the optical sense which passes through two points A and B in a medium having an index n(xyz) varying from one point to another but constant in time is such that the integral A I B nd2 taken along this ray is extreme. On the other hand Maupertuis’ principle of least action teaches us the following: the trajectory of a corpuscle passing through two points A and B in space is such that the integral I “pdl A taken along the trajectory is extreme, provided, of course, that only the motions corresponding to a given energy value are considered. From the relations derived above between the mechanical and the wave parameters, we have:

WAVE NATURE OF ELECTRON 251 since W is constant in a constant field. It follows that Fermats and maupe tuis principles are each a translation of the other and the possible trajectories of the corpuscle are identical to the possible rays of its wave These concepts lead to an interpretation of the conditions of stability in- troduced by the quantum theory. Actually, if we consider a closed trajectory C in a constant field, it is very natural to assume that the phase of the asso ciated wave must be a uniform function along this trajectory. Hence we may write ∫=∫ d integer This is precisely Plancks condition of stability for periodic atomic motions The conditions of quantum stability thus emerge as analogous to resonance phenomena and the appearance of integers becomes as natural here as in the theory of vibrating cords and plates The general formulae which establish the parallelism between waves corpuscles may be applied to corpuscles of light on the assumption that the rest mass mo is infinitely small. Actually, if for a given value of energy W, mo is made to tend towards zero, u and V are both found to tend towards c and at the limit the two fundamental formulae are obtained on which Einstein had based his light-quantum theory W=hy Such are the main ideas which I developed in my initial studies. They showed clearly that it was possible to establish a correspondence between waves and orpuscles such that the laws of mechanics correspond to the laws of geomet- rical optics. In the wave theory, however, as you will know, geometrical and particularly when interference and diffraction phenomena are involved, it is quite inadequate. This prompted the thought that classical mechanics is also only an approximation relative to a vaster wave mechanics. I stated as much almost at the outset of my studies, ie. "A new mechanics must be developed which is to classical mechanics what wave optics is to geomet- ical optics". This new mechanics has since been developed, thanks mainly

WAVE NATURE OF ELECTRON 251 since W is constant in a constant field. It follows that Fermat’s and Mauper￾tuis’ principles are each a translation of the other and the possible trajectories of the corpuscle are identical to the possible rays of its wave. These concepts lead to an interpretation of the conditions of stability in￾troduced by the quantum theory. Actually, if we consider a closed trajectory C in a constant field, it is very natural to assume that the phase of the asso￾ciated wave must be a uniform function along this trajectory. Hence we may write : This is precisely Planck’s condition of stability for periodic atomic motions. The conditions of quantum stability thus emerge as analogous to resonance phenomena and the appearance of integers becomes as natural here as in the theory of vibrating cords and plates. The general formulae which establish the parallelism between waves and corpuscles may be applied to corpuscles of light on the assumption that here the rest mass m. is infinitely small. Actually, if for a given value of the energy W, m. is made to tend towards zero, v and V are both found to tend towards c and at the limit the two fundamental formulae are obtained on which Einstein had based his light-quantum theory Such are the main ideas which I developed in my initial studies. They showed clearly that it was possible to establish a correspondence between waves and corpuscles such that the laws of mechanics correspond to the laws of geomet￾rical optics. In the wave theory, however, as you will know, geometrical optics is only an approximation: this approximation has its limits of validity and particularly when interference and diffraction phenomena are involved, it is quite inadequate. This prompted the thought that classical mechanics is also only an approximation relative to a vaster wave mechanics. I stated as much almost at the outset of my studies, i.e. "A new mechanics must be developed which is to classical mechanics what wave optics is to geomet￾rical optics". This new mechanics has since been developed, thanks mainly

1929 L DE BROGLIE to the fine work done by Schrodinger. It is based on wave propagation equations and strictly defines the evolution in time of the wave associated with a corpuscle. It has in particular succeeded in giving a new and more satisfactory form to the quantization conditions of intra-atomic motion since he classical quantization conditions are justified, as we have seen, by the pplication of geometrical optics to the waves associated with the intra atomic corpuscles, and this application is not strictly justified I cannot attempt even briefly to sum up here the development of the new mechanics. I merely wish to say that on examination it proved to be iden- tical with a mechanics independently developed, first by Heisenberg, then by Born, Jordan, Pauli, Dirac, etc. quantum mechanics. The two mechan- ics, wave and quantum, are equivalent from the mathematical point of vIew We shall content ourselves here by considering the general significance of the results obtained. To sum up the meaning of wave mechanics it can be stated that: "A wave must be associated with each corpuscle and only the study of the waves propagation will yield information to us on the succes sive positions of the corpuscle in space". In conventional large-scale mechani cal phenomena the anticipated positions lie along a curve which is the trajec- tory in the conventional meaning of the word. But what happens if the wave does not propagate according to the laws of optical geometry, if, say, there are interferences and diffraction? Then it is no longer possible to assign to the corpuscle a motion complying with classical dynamics, that much is certain Is it even still possible to assume that at each moment the corpuscle occupies a well-defined position in the wave and that the wave in its propagation car ries the corpuscle along in the same way as a wave would carry along a cork? These are difficult questions and to discuss them would take us too far and even to the confines of philosophy. All that I shall say about them here is that nowadays the tendency in general is to assume that it is not constantly pos- the corpuscle a well-defined position in the wave. I must restrict myself to the assertion that when an observation is carried out en abling the localization of the corpuscle, the observer is invariably induced to assign to the corpuscle a position in the interior of the wave and the the square of the amplitude, that is to say the intensity al proportional to probability of it being at a particular point M of the wave is This may be expressed in the following If we consider a cloud of corpuscles associated with the same wave, the intensity of th e wave at ea point is proportional to the cloud density at that point(ie to the number of

252 1929 L.DE BROGLIE to the fine work done by Schrödinger. It is based on wave propagation equations and strictly defines the evolution in time of the wave associated with a corpuscle. It has in particular succeeded in giving a new and more satisfactory form to the quantization conditions of intra-atomic motion since the classical quantization conditions are justified, as we have seen, by the application of geometrical optics to the waves associated with the intra￾atomic corpuscles, and this application is not strictly justified. I cannot attempt even briefly to sum up here the development of the new mechanics. I merely wish to say that on examination it proved to be iden￾tical with a mechanics independently developed, first by Heisenberg, then by Born, Jordan, Pauli, Dirac, etc.: quantum mechanics. The two mechan￾ics, wave and quantum, are equivalent from the mathematical point of view. We shall content ourselves here by considering the general significance of the results obtained. To sum up the meaning of wave mechanics it can be stated that: "A wave must be associated with each corpuscle and only the study of the wave’s propagation will yield information to us on the succes￾sive positions of the corpuscle in space". In conventional large-scale mechani￾cal phenomena the anticipated positions lie along a curve which is the trajec￾tory in the conventional meaning of the word. But what happens if the wave does not propagate according to the laws of optical geometry, if, say, there are interferences and diffraction? Then it is no longer possible to assign to the corpuscle a motion complying with classical dynamics, that much is certain. Is it even still possible to assume that at each moment the corpuscle occupies a well-defined position in the wave and that the wave in its propagation car￾ries the corpuscle along in the same way as a wave would carry along a cork? These are difficult questions and to discuss them would take us too far and even to the confines of philosophy. All that I shall say about them here is that nowadays the tendency in general is to assume that it is not constantly pos￾sible to assign to the corpuscle a well-defined position in the wave. I must restrict myself to the assertion that when an observation is carried out en￾abling the localization of the corpuscle, the observer is invariably induced to assign to the corpuscle a position in the interior of the wave and the probability of it being at a particular point M of the wave is proportional to the square of the amplitude, that is to say the intensity at M. This may be expressed in the following manner. If we consider a cloud of corpuscles associated with the same wave, the intensity of the wave at each point is proportional to the cloud density at that point (i.e. to the number of

WAVE NATURE OF ELECTRON orpuscles per unit volume around that point). This hypothesis is necessary to explain how, in the case of light interferences, the light energy is con- centrated at the points where the wave intensity is maximum: if in fact it is assumed that the light energy is carried by light corpuscles, photons, then the photon density in the wave must be proportional to the intensity This rule in itselfwill enable us to understand how it was possible to verify the wave theory of the electron by experiment Let us in fact imagine an indefinite cloud of electrons all moving at the ame velocity in the same direction. In conformity with the fundamental ideas of wave mechanics we must associate with this cloud an indefinite plane wave of the form 「W,xx+By+ asmn2元 Lh where apy are the cosines governing the propagation direction and where he wavelength A is equal to ly/p. With electrons which are not extremely d hend where mo is the rest mass of the electron You will be aware that in practice, to obtain electrons moving at the same velocity, they are made to undergo a drop in potential P and we have h lly this gives I2.24 10-8 cm (Pin volts)

WAVE NATURE OF ELECTRON 253 corpuscles per unit volume around that point). This hypothesis is necessary to explain how, in the case of light interferences, the light energy is con￾centrated at the points where the wave intensity is maximum: if in fact it is assumed that the light energy is carried by light corpuscles, photons, then the photon density in the wave must be proportional to the intensity. This rule in itselfwill enable us to understand how it was possible to verify the wave theory of the electron by experiment. Let us in fact imagine an indefinite cloud of electrons all moving at the same velocity in the same direction. In conformity with the fundamental ideas of wave mechanics we must associate with this cloud an indefinite plane wave of the form where aby are the cosines governing the propagation direction and where the wavelength 1, is equal to h/p. With electrons which are not extremely fast, we may write and hence where m. is the rest mass of the electron. You will be aware that in practice, to obtain electrons moving at the same velocity, they are made to undergo a drop in potential P and we have Hence, Numerically this gives