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Quantum-mechanical treatment of two particles in a potential box

  • Gottfried Mann EMAIL logo
Veröffentlicht/Copyright: 23. Januar 2024
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Zeitschrift für Naturforschung A
Aus der Zeitschrift Zeitschrift für Naturforschung A Band 79 Heft 5

Abstract

In classical physics, there is a basic principle, namely “A particle cannot be located at the position of another one on the same time.” Which consequences can be derived if this principle is transferred into quantum physics? For doing that, two distinguishable particles are considered to be trapped in a potential box by means of the Schrödinger equation. In result, the particles can necessarily be located only at discrete positions.

Keywords: two particles in a potential box; Schrödinger equation; discrete positions

1 Introduction

In classical physics, there is a basic principle, which is called “Where a body is located, another one cannot be there at the same time.” (see e.g., [1] as a textbook). In the present paper, it is discussed what results from this principle, if it is transferred into quantum physics. For doing that, two distinguishable, impenetrable, pointlike particles trapped in a potential box are considered in terms of quantum mechanics. For this case, the stationary one-dimensional Schrödinger equation (see e.g., [2] as a textbook) can be written as

(1) E ⋅ ψ ( x 1 , x 2 ) = − ℏ 2 2 m 1 2 ⋅ ∂ 2 ψ ∂ x 1 2 − ℏ 2 2 m 2 2 ⋅ ∂ 2 ψ ∂ x 2 2 + V box ( x 1 ) ⋅ ψ + V box ( x 2 ) ⋅ ψ + V int ( x 1 , x 2 ) ⋅ ψ

(ℏ = h/2π with Planck’s constant h) with E as the energy of the two-particle system. m 1 and m 2 denote the masses of the 1st and 2nd particle, respectively. The wave function ψ(x 1, x 2) is depending on the spatial coordinates x 1 and x 2 of the 1st and 2nd particle, respectively. V box (x) describes the potential of the potential box with the spatial length L:

(2) V box ( x ) = 0   for   0 < x < L ∞   otherwise

(Here, x should be taken either for x 1 or for x 2.) As argued above, one particle cannot be at the position of the other one on the same time. That can be regarded as some kind of interaction, which is described by the potential[1]

(3) V int ( x 1 , x 2 ) = ∞     for   x 1 = x 2 0     for   x 1 ≠ x 2

In quantum mechanics, ‖ψ(x 1, x 2)‖2 ⋅dx 1dx 2 gives the probability that the 1st and 2nd particle are located in the intervals (x 1, x 1 + dx 1) and (x 2, x 2 + dx 2), respectively (see e.g., [2]). Because of this meaning of the wave function, the inclusion of the potential V int into Eq. (1) leads to the requirement that the wave function must vanish for x 1 = x 2 (see for more details Appendix A). There, a particle is considered in a potential box in which an infinitely thin and high potential wall is additionally inserted at the position x = 0. It is shown that the wave function has consequently a zero there.

Thus, the task to be discussed is completely defined by Eqs. (1)–(3).

2 Classical solution in quantum mechanics

The treatment of a particle in the potential box is a classical task in textbooks of quantum mechanics (see [2], [3] and also Appendix A). Now, the case in which both particles are trapped in the potential box without any interaction is considered, i.e., the potential V int is neglected. Then, Eq. (1) reduces to

(4) E ⋅ ψ ( x 1 , x 2 ) = − ℏ 2 2 m 1 2 ⋅ ∂ 2 ψ ∂ x 1 2 − ℏ 2 2 m 2 2 ⋅ ∂ 2 ψ ∂ x 2 2 + V box ( x 1 ) ⋅ ψ + V box ( x 2 ) ⋅ ψ

The potential V box requires that the wave function ψ(x 1, x 2) vanishes at the walls of the potential box and outside of the region 0 < x 1, x 2 < L. Then, the solution of Eq. (4) is found to be

(5) ψ ( x 1 , x 2 ) = 2 L ⋅ sin ( k 1 x 1 ) ⋅ sin ( k 2 x 2 )

with

(6) k 1 = 2 m 1 E 1 ℏ = n 1 ⋅ π L

(7) k 2 = 2 m 2 E 2 ℏ = n 2 ⋅ π L

(n 1, n 2 = 1, 2, 3, …) and

(8) E = E 1 + E 2 = ℏ 2 k 1 2 2 m 1 + ℏ 2 k 2 2 2 m 2

in the region 0 < x 1, x 2 < L. Note, that the wave function is normalized to unity and is a real one, here. E 1 and E 2 denote the energies of the 1st and 2nd particle, respectively.

3 Inclusion of the potential V int

The wave function (Eq. (5)) is adopted for describing both particles in the potential box. The potential V int(x 1, x 2) (see Eq. (3)) describes the interaction of both particles with each other. As discussed in Section 1, the wave function (Eq. (5)) must have a zero at x 1 = x 2 because of the potential V int leading to

(9) cos [ ( k 1 − k 2 ) x 2 ] = cos [ ( k 1 + k 2 ) x 2 ]

This equation is fulfilled for β = 2πν 1 + α and/or β = 2πν 2 − α with α = (k 1 − k 2)x 2 and β = (k 1 + k 2)x 2 and ν 1, ν 2 = 1, 2, 3, …, leading to α + β = 2k 1 x 2 = 2πν 2 and

(10) x 2 = ν 2 π k 1 = ν 2 n 1 ⋅ L

with ν 2 ≤ n 1 because of x 2 ≤ L. (Here, Eq. (6) has been used.) For x 2 → x 1, the same procedure provides

(11) x 1 = ν 1 π k 2 = ν 1 n 2 ⋅ L

with ν 1 ≤ n 2.

According to Eqs. (10) and (11), the nearest positions of the 1st and 2nd particle to the potential wall at x = L are x 2 = [(n 1 − 1)/n 1]L and x 1 = [(n 2 − 1)/n 2]L, respectively. Then, the distance between these positions are found to be

(12) ‖ x 1 − x 2 ‖ L = ‖ n 2 − n 1 ‖ n 1 n 2 ⋅ 1 L

Hence, the distance of two neighboring positions of the 1st and 2nd particle becomes smaller for n 1, n 2 → ∞ but never exactly zero as it should be, taking into account n 1 ≠ n 2. Note, that, as well-known, quantum-mechanical results transfer into the classical ones for large quantum numbers, i.e., n 1, n 2 → ∞. In the regime of classical mechanics, all positions in the box have the same probability to be occupied by the particles as discussed in Appendix B.

Inserting Eqs. (10) and (11) into Eq. (5), the wave function has the form

(13) ψ ( x 1 , x 2 ) = 4 L 2 ⋅ sin ν 1 , i n 2 n 1 π ⋅ sin ν 2 , j n 1 n 2 π

with ν 1,i = 1, …, n 2 and ν 2,j = 1, …, n 1. Now, the wave function ψ is actually not a function but a matrix. According to the interpretation of the wave function in quantum mechanics, the matrix W i , j ∝ W ̃ i , j = ‖ ψ ‖ 2 gives the probability that the 1st and 2nd particle are located at the ith and jth position, respectively. That leads to

(14) W ̃ i , j = 4 L 2 ⋅ sin 2 ν 1 n 2 n 1 π ⋅ sin 2 ν 2 n 1 n 2 π

Since W i,j should be normalized to unity, i.e.,

(15) ∑ i , j W ̃ i , j = 1

one finds for

(16) W i , j = W ̃ i , j ∑ i , j W ̃ i , j

Now, the matrix W i,j is completely determined by Eqs. (14)–(16).

In result, the appearance of a second particle in the potential box and the principle, that a particle cannot be at a place of the other one at the same time, leads consequently to the fact that both particles can only be located at discrete positions in the potential box with individual probabilities, which are always smaller than unity.

4 An example

For illustrating the procedure presented in the previous section, a special example will be discussed. Low quantum states are chosen, namely n 1 = 3 and n 2 = 4, for instance. Hence, 3 and 2 positions are disposable for the 1st and 2nd particle, respectively, i.e.,

(17) x 11 = L 4 x 12 = L 2 x 13 = 3 L 4

and

(18) x 21 = L 3 x 22 = 2 L 3

x 1i and x 2j denote the positions of the 1st and 2nd particle, respectively. W ̃ i j = ‖ ψ ( x 1 i , x 2 j ) ‖ 2 are the relative probabilities that the 1st and 2nd particle take the ith and jth positions, respectively. Hence, one gets 2 × 3 elements for the matrix

(19) W ̃ i j = 4 L 2 ⋅ sin 2 ν 1 i 4 ⋅ 3 π ⋅ sin 2 ν 2 j 3 ⋅ 4 π

with ν 1i = 1, 2, 3 and ν 2j = 1, 2. For instance, one finds for W ̃ 1,2 ∝ sin 2 ( 3 π / 4 ) ⋅ sin 2 ( 8 π / 3 ) = 3 / 8 . Following this procedure and taking into account Eqs. (15), (17), and (18), the matrix of probability (see Eq. (16)) is found to be

(20) W i j = 1 / 8 1 / 8 1 / 4 1 / 4 1 / 8 1 / 8

With the knowledge of the matrix W ij , the mean positions of the 1st and 2nd particle within the potential box can be calculated to be x ̄ 1 = L / 2 and x ̄ 2 = L / 2 , respectively, according to

(21) x ̄ 1 = ∑ i , j x 1 i ⋅ W i j   and   x ̄ 2 = ∑ i , j x 2 i ⋅ W i j

Both values agree with the value of the classical approach (see Eq. (49)) as presumed. The mean square ( Δ x 1 ) 2 ̄ of the fluctuations of the positions of the 1st particle around its mean value x ̄ 1 is defined by

(22) ( Δ x 1 ) 2 ̄ = x 1 2 ̄ − ( x ̄ 1 ) 2

with

(23) x 1 2 ̄ = ∑ i , j x 1 i 2 ⋅ W i j

Following this procedure, one finds ( Δ x 1 ) 2 ̄ / L 2 = 1/32 and ( Δ x 2 ) 2 ̄ / L 2 = 1/36 for the 1st and 2nd particle, respectively. Both values are smaller than the value of 1/12 (see Eq. (52)) in the classical approach.

The distances of neighboring positions of the 1st and 2nd particle are L/12, 5L/12, and/or L/6 taking into account Eqs. (17) and (18). The mean distance d ̄ between both particles is defined by

(24) d ̄ = ∑ i , j ‖ x 1 i − x 2 j ‖ ⋅ W i j

and is calculated to be d ̄ / L = 5 / 24 ( ≈ 0.2083 ) . Note, that the classical approach provides for d ̄ / L = 1 / 3 (see Eq. (54)). Then, the mean square ( Δ d ) 2 ̄ / L 2 of the fluctuation of the distance d around the mean value d ̄ is found to be ( Δ d ) 2 ̄ / L 2 = 1 / 64 ( ≈ 0.0156 ) by means of

(25) ( Δ d ) 2 ̄ = d 2 ̄ − ( d ̄ ) 2

and

(26) d 2 ̄ = ∑ i , j ‖ x 1 i − x 2 j ‖ 2 ⋅ W i j .

This value is smaller than 1/18, which is the value of the classical approach (see Eq. (56)).

In the case of discussion, the derived values of ( Δ x 1 ) 2 ̄ / L 2 , ( Δ x 2 ) 2 ̄ / L 2 , d ̄ , and ( Δ d ) 2 ̄ / L 2 are smaller than those of the classical approach (see Appendix B). That can be explained in the following manner: As already mentioned, ‖ψ(x 1, x 2)‖2 gives the density of probability that the 1st and 2nd particle are located in the intervals (x 1, x 1 + dx 1) and (x 2, x 2 + dx 2), respectively (see [2] as a textbook). Since ‖ψ‖2 ∝ sin2(k 1 x 1) ⋅ sin2(k 2 x 2) (see Eq. (5)), this probability is greater in the middle of the box than at its edges. Thus, one can say that the walls of the potential box acts like a repulsive force on the particle. That is a pure quantum-mechanical effect, since it does not appear in classical physics (see Appendix B). Since both particles are more located at the middle of the box, consequently, their distance to each other becomes also smaller in comparison to the classical approach (see Appendix B).

In Section 3, it has been shown that the particles are localized at discrete positions, This result seems to contradict to Heisenberg’s inequality (see [2]). But it is not the case as demonstrated in the framework of the example discussed in this section: In quantum mechanics, the momentum p is given by p = ℏk ([2]) with k as the wave number. In the case of a particle with the mass m trapped in a potential box, one finds p ̄ = 0 and ( Δ p ) 2 ̄ = ( ℏ k ) 2 (see [3]). The 1st particle has the quantum number n 1 = 3 leading to ( Δ p 1 ) 2 ̄ = ( 9 ℏ π / L ) 2 (see Eq. (6)), ( Δ x 1 ) 2 ̄ = 1 / 32 , and, finally, to ( Δ p ) 2 ̄ ⋅ ( Δ x 1 ) 2 ̄ = ( 81 π 2 ℏ 2 / 32 ) ≥ ℏ 2 / 4 . A similar result is obtained for the 2nd particle by the same procedure. Hence, the results presented in this paper does not contradict to Heisenberg’s inequality, as it should be.

5 Summary

In this paper, the basic principle of classical physics, namely “A particle cannot be located at the position of another one on the same time” (see e.g., [1] as a textbook), is transferred into quantum mechanics. For doing that, two distinguishable particles with different masses trapped in a potential box are considered in the framework of quantum mechanics. This task is treated by means of the stationary one-dimensional Schrödinger equation.

In Appendix A, the problem of one particle in the potential box is studied with an additional insertion of an infinitely thin wall with an infinitely high potential at the position x = 0. In quantum mechanics, the particle can penetrate through the wall due to the “tunnel effect” [3], but its wave function must have necessarily a zero at x = 0 as shown in Appendix A.

In order to describe that one particle cannot be located at the place of the other one at the same time, the potential V int (see Eq. (3)) is introduced in Eq. (1). It is infinite at x 1 = x 2 and zero otherwise as defined by Eq. (3). According to the result in Appendix A, the wave function ψ(x 1, x 2) must have a zero at x 1 = x 2. Consequently, both particles must be located at individual discrete positions as discussed in Section 3. Hence, the wave function ψ has to be substituted by a matrix W i,j . This matrix W i,j gives the probability that the 1st and 2nd particle are located at the positions x 1,i and x 2,j , respectively, as demonstrated in terms of an example in Section 4.

In order to avoid misunderstandings, it should be emphasized that the approach presented in this paper has nothing to do with “fermions” and “bosons,” which are basically indistinguishable particles. Here, two particles with different masses, i.e., distinguishable particles, are considered to be trapped in a potential box. The addition of a second particle in the potential box leads inevitably to a discretization of the locations of the particles in the box if one takes into account that an individual particle cannot be at the position of the other ones at the same time. It should be emphasized that the location of the particles at discrete positions does not violate Heisenberg’s inequality as demonstrated in Section 4. They are localized at discrete positions with different probabilities, which are nowhere unity.

Corresponding author: Gottfried Mann, Leibniz-Institut für Astrophysik Potsdam (AIP), An der Sternwarte 16, D-14482 Potsdam, Germany, E-mail:

Acknowledgments

As mentioned in the Acknowledgments of the manuscript, the author is grateful to Dr. Hakan Önel for his LATEX support during the preparation of the manuscript ZNA.2023.0157.

  1. Research ethics: Not applicable.

  2. Author contributions: The author has accepted responsibility for the entire content of manuscript ZNA.2023.0157 and approved its submission.

  3. Competing interests: The author state no competing interests.

  4. Research funding: None declared.

  5. Data availability: Not applicable.

A Quantum-mechanical treatment of a single particle in a one-dimensional potential box with a potential wall

A single particle with the mass m and the energy E is considered to be trapped in the potential box with the length L. Additionally, a potential wall of the width b is inserted at x = 0. Then, the stationary one-dimensional Schrödinger equation of this problem is written as

(27) − ℏ 2 2 m ⋅ d 2 ⁡ ψ d x 2 + V box ψ + V wall ψ = E ⋅ ψ ( x )

V box describes the potential of the box as given by

(28) V box ( x ) = 0   for − L / 2 < x < L ∞   otherwise

The potential wall with the spatial width b is inserted at x = 0. Its potential V wall is described by

(29) V wall ( x ) = V 0   for − b / 2 < x < b / 2 0   otherwise

Now, the inclusion of the potential wall at the position x = 0 within the box is considered. (Here, we follow the procedure presented in [3] p. 94). Then, the wave function ψ(x) has the general form

(30) ψ = A ⁡ sin ( k x ) + B ⁡ cos ( k x )   at − L / 2 < x < − b / 2   C e − κ x + D e κ x   at − b / 2 ≤ x ≤ b / 2   E ⁡ sin ( k x ) + F ⁡ cos ( k x )   at + b / 2 < x < L  

with

(31) k = 2 m E / ℏ

and

(32) κ = 2 m ( V 0 − E ) / ℏ

Here, V 0 > E is generally assumed, so that k and κ are real and positive quantities.

The task to be treated is symmetrical with respect to x = 0. Consequently, the resulted wave function ψ(x) is either symmetrical or antisymmetrical. The symmetrical and antisymmetrical cases are given by A = E = 0 and C = D, and B = F = 0 and C = −D, respectively. Because of the shape of V box , the wave function ψ must vanish at x = ±L/2. That leads to

(33) k n = ( 2 n − 1 ) π L     for   n = 1 ; 2 ; 3 ; …

and

(34) k n = 2 n π L     for   n = 1 ; 2 ; 3 ; …

for the symmetrical and antisymmetrical cases, respectively.

The wave function and its first derivation with respect to x must be continuous at x = ±b/2 (see [3]). In the symmetrical case, it leads to

(35) B ⋅ cos ( k b / 2 ) = C ⋅ e κ b / 2 + e − κ b / 2

and

(36) k B ⋅ sin ( k d / 2 ) = − κ C ⋅ e κ d / 2 − e − κ d / 2

at x = −b/2. Eqs. (35) and (36) represent a homogeneous system of equations with the determinant

(37) k κ ⋅ sin ( k b / 2 ) = − cos ( k b / 2 ) ⋅ e κ b / 2 − e − κ b / 2 e κ b / 2 + e − κ b / 2

As considered here, the potential wall has an infinitely high potential and an infinitely thin width. It means k/κ ≪ 1 (because of V 0 ≫ E) and kb ≪ 1. Under these conditions, the left hand side of Eq. (37) vanishes, whereas the right hand site of it does it only for κb = 0. Hence, there are no symmetrical solutions of the task for arbitrary values of κb. In the antisymmetrical case, Eqs. (38) and (39)

(38) − A ⋅ sin ( k b / 2 ) = C ⋅ e κ b / 2 − e − κ b / 2

and

(39) k A ⋅ cos ( k b / 2 ) = − κ C ⋅ e κ b / 2 + e − κ b / 2

results from the requirement of continuity of the wave function and its first derivative with respect to x at x = −b/2

(40) B ⋅ cos ( k b / 2 ) = C ⋅ e κ b / 2 + e − κ b / 2

and

(41) k B ⋅ sin ( k d / 2 ) = − κ C ⋅ e κ b / 2 − e − κ b / 2

at x = −b/2. The determinant of this homogeneous system of equations (see Eqs. (40) and (41)) is found to be

(42) k κ ⋅ cos ( k d / 2 ) = sin ( k d / 2 ) ⋅ e κ d / 2 + e − κ d / 2 e κ d / 2 − e − κ d / 2

The denominator in the right hand side of Eq. (42) has a zero for κb = 0. Expanding the left and right hand sides of Eq. (42) with respect to k/κ ≪ 1 and κb ≪ 1, one gets

(43) k κ ≈ k d 2 ⋅ 2 κ d = k κ ≪ 1

Thus, Eq. (42) can be fulfilled well by the conditions k/κ ≪ 1 and kd ≪ 1. Hence, the antisymmetric wave function is a solution of the considered task. This wave function has consequently a zero at x = 0, where the potential wall is located. The energy of the quantum state n is given by E = ( ℏ k n ) 2 / 2 m (see Eq. (8)). Due to the insertion of the potential wall, the energy of the ground state is enhanced from E = (ℏπ/L)2/2m (before the insertion) to E = 4 × (ℏπ/L)2/2m (after the insertion). Thus, the potential wall acts on the particle like a repulsive force.

Atkinson & Crater [4] and Busch et al. [5] considered the effects of an additional delta-function potential in bound states, as for instance for a potential box and a harmonic potential, in terms of the stationary Schrödinger equation. In the case of the potential box, as discussed here, the delta-function was added in the middle of the box (see [4]). Symmetric solutions with a nonvanishing value at the position of the delta-function were found. This result contradicts to our result presented in this section. The reason may be that the potential of the wall (see Eq. (29)) does not agree with a delta-function, since the delta-function is not actually a function but a distribution.2

B Classical approach of two particles in a potential box

A particle is considered to be trapped in a one-dimensional potential box as defined by Eq. (2). In the framework of classical mechanics, all positions in the interval 0 < x < L have the same probability to be occupied by the particle. Hence, the density of probability w 1 that the particle is located in the interval (x, x + dx) is constant in the box. It is given by

(48) w 1 ( x ) = 1 / L   for   0 < x < L 0   otherwise

Note that w 1 is normalized to unity, as it should be. Hence, the mean location of the particle is found to be

(49) x ̄ = ∫ d x ⋅ x ⋅ w 1 ( x ) = 1 L ⋅ ∫ 0 L d x ⋅ x = L 2

as presumed. The mean square ( Δ x ) 2 ̄ of the fluctuations of the position of the particle around its mean value (i.e., x ̄ = L / 2 ) is defined by

(50) ( Δ x ) 2 ̄ = x 2 ̄ − ( x ̄ ) 2

with

(51) x 2 ̄ = ∫ d x ⋅ x 2 ⋅ w 1 ( x ) = L 2 3

leading to

(52) ( Δ x ) 2 ̄ = L 2 12

In the next step, the case of two particles trapped in the potential box is discussed. As before, all positions x 1 and x 2 in the interval 0 < x 1, x 2 < L have the same probability for both particles. Here, x 1 and x 2 denote the spatial coordinates of the 1st and 2nd particle, respectively. Then, the density of probability that the 1st and 2nd particle are located in the interval (x 1, x 1 + dx 1) and (x 2, x 2 + dx 2), respectively, is given by

(53) w 2 ( x 1 , x 2 ) = 1 / L 2   for   0 < x < L 0   otherwise

Note that w 2 is normalized to unity. The mean distance d ̄ between both particles is defined by

(54) d ̄ = ∫ d x 1 d x 2 ⋅ ‖ x 1 − x 2 ‖ ⋅ w 2 ( x 1 , x 2 ) = L 3

Such a value is expected, since both particles have the same distance to the walls of the potential box and to each other in the mean sense. In order to obtain the mean square ( Δ d ) 2 ̄ of the fluctuations of the distance d between both particles around its mean value d ̄ , the quantity

(55) d 2 ̄ = ∫ d x 1 d x 2 ⋅ ‖ x 1 − x 2 ‖ 2 ⋅ w 2 ( x 1 , x 2 ) = L 2 6

has to be calculated. Then, one finds for

(56) ( Δ d ) 2 ̄ = d 2 ̄ − ( d ̄ ) 2 = L 2 6 − L 2 9 = L 2 18

References

[1] D. Meschede, Gerthsen – Physics, Berlin, Heidelberg, Springer Verlag, 2015.10.1007/978-3-662-45977-5Suche in Google Scholar

[2] L. D. Landau and E. M. Lifschitz, Quantenmechanik, vol. III, Berlin, Akademie Verlag, 1974.Suche in Google Scholar

[3] A. S. Dawydow, Quantenmechanik, Berlin, Deutscher Verlag der Wissenschaften, 1978.Suche in Google Scholar

[4] D. A. Atkinson and H. W. Crater, “An exact treatment of the Dirac delta function potential in the Schrödinger equation,” Am. J. Phys., vols. 43/4, p. 301, 1973. https://doi.org/10.1119/1.9857.Suche in Google Scholar

[5] T. Busch, B.-G. Englert, K. Rzazewski, and M. Wilkens, “Two cold atoms in a harmonic trap,” Found. Phys., vol. 28, no. 4, p. 549, 1998https://doi.org/10.1023/a:1018705520999.10.1023/A:1018705520999Suche in Google Scholar

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Received: 2023-06-21
Accepted: 2023-12-31
Published Online: 2024-01-23
Published in Print: 2024-05-27

© 2024 the author(s), published by De Gruyter, Berlin/Boston

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  2. General
  3. Magnetoacoustics and magnetic quantization of Fermi states in relativistic plasmas
  4. Atomic, Molecular & Chemical Physics
  5. Investigations on the EPR parameters and local structures for the substitutional Ti3+ and W5+ centers in stishovite
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https://doi.org/10.1515/zna-2023-0157
Schlagwörter für diesen Artikel
two particles in a potential box; Schrödinger equation; discrete positions
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Artikel in diesem Heft

  1. Frontmatter
  2. General
  3. Magnetoacoustics and magnetic quantization of Fermi states in relativistic plasmas
  4. Atomic, Molecular & Chemical Physics
  5. Investigations on the EPR parameters and local structures for the substitutional Ti3+ and W5+ centers in stishovite
  6. Dynamical Systems & Nonlinear Phenomena
  7. The effects of viscosity on the structure of shock waves in a van der Waals gas
  8. Traveling wavefronts in an anomalous diffusion predator–prey model
  9. Bifurcation and stability analysis of atherosclerosis disease model characterizing the anti-oxidative activity of HDL during short- and long-time evolution
  10. Nuclear Physics
  11. Investigation of 90,92Zr(n,γ)91,93Zr in the s-process nucleosynthesis
  12. Quantum Theory
  13. Quantum-mechanical treatment of two particles in a potential box
  14. Solid State Physics & Materials Science
  15. Unveiling the luminescence property of Pr-incorporated barium cerate perovskites for white LED applications
  16. Electrical and magnetic properties of MF/CuAl nanocomposites
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