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Research Article

Effect of Mth coherent state on the interaction between two two-level atoms and two-mode quantized field

ORCID Icon &
Pages 1053-1064 | Received 11 Apr 2022, Accepted 23 Oct 2022, Published online: 05 Nov 2022

Figures & data

Figure 1. The atomic inversion for asymmetric two atoms (g=g1/g2=0.5) at δ=0, λ=1; cases (A–D) black for M1=M2=0, blue for M1=M2=20, red for M1=M2=40, and green for M1=M2=60; while cases (E–H) black for M1=60 and M2=0, blue for M1=0 and M2=60, red for M1=40 and M2=20 and green for M1=20 and M2=40. (A) First Atom; (B) First Atom; (C) Second Atom; (D) Second Atom; (E) First Atom; (F) First Atom; (G) Second Atom; (H) Second Atom.

Figure 1. The atomic inversion for asymmetric two atoms (g=g1/g2=0.5) at δ=0, λ=1; cases (A–D) black for M1=M2=0, blue for M1=M2=20, red for M1=M2=40, and green for M1=M2=60; while cases (E–H) black for M1=60 and M2=0, blue for M1=0 and M2=60, red for M1=40 and M2=20 and green for M1=20 and M2=40. (A) First Atom; (B) First Atom; (C) Second Atom; (D) Second Atom; (E) First Atom; (F) First Atom; (G) Second Atom; (H) Second Atom.

Figure 2. The atomic inversion for symmetric two atoms (g=g1/g2=1) at δ=0, λ=1; cases (A–B) black for M1=M2=0, blue for M1=M2=20, red for M1=M2=40 and green for M1=M2=60, while cases (C–D) black for M1=60 and M2=0, blue for M1=0 and M2=60, red for M1=40 and M2=20 and green for M1=20 and M2=40.

Figure 2. The atomic inversion for symmetric two atoms (g=g1/g2=1) at δ=0, λ=1; cases (A–B) black for M1=M2=0, blue for M1=M2=20, red for M1=M2=40 and green for M1=M2=60, while cases (C–D) black for M1=60 and M2=0, blue for M1=0 and M2=60, red for M1=40 and M2=20 and green for M1=20 and M2=40.

Figure 3. The von Neumann entropy for asymmetric two atoms (g = 0.5) at δ=0, λ=1; cases (A–D) black for M1=M2=0, blue for M1=M2=20, red for M1=M2=40, and green for M1=M2=60; while cases (E–H) black for M1=60 and M2=0, blue for M1=0 and M2=60, red for M1=40 and M2=20 and green for M1=20 and M2=40. (A) First Atom; (B) First Atom; (C) Second Atom; (D) Second Atom; (E) First Atom; (F) First Atom; (G) Second Atom; (H) Second Atom.

Figure 3. The von Neumann entropy for asymmetric two atoms (g = 0.5) at δ=0, λ=1; cases (A–D) black for M1=M2=0, blue for M1=M2=20, red for M1=M2=40, and green for M1=M2=60; while cases (E–H) black for M1=60 and M2=0, blue for M1=0 and M2=60, red for M1=40 and M2=20 and green for M1=20 and M2=40. (A) First Atom; (B) First Atom; (C) Second Atom; (D) Second Atom; (E) First Atom; (F) First Atom; (G) Second Atom; (H) Second Atom.

Figure 4. The y-component of the variance squeezing for asymmetric two atoms (g = 0.5) at δ=0, λ=1; cases in the second column are the same cases in first column with different time. (A) First Atom; (B) First Atom; (C) Second Atom; (D) Second Atom; (E) First Atom; (F) First Atom; (G) Second Atom; (H) Second Atom.

Figure 4. The y-component of the variance squeezing for asymmetric two atoms (g = 0.5) at δ=0, λ=1; cases in the second column are the same cases in first column with different time. (A) First Atom; (B) First Atom; (C) Second Atom; (D) Second Atom; (E) First Atom; (F) First Atom; (G) Second Atom; (H) Second Atom.

Figure 5. The correlation function for asymmetric two atoms (g = 0.5) at δ=0, λ=1; cases in the second column are the same cases in first column with different time. (A) First mode quantized field; (B) First mode quantized field; (C) Second mode quantized field; (D) Second mode quantized field; (E) First mode quantized field; (F) First mode quantized field; (G) Second mode quantized field; (H) Second mode quantized field.

Figure 5. The correlation function for asymmetric two atoms (g = 0.5) at δ=0, λ=1; cases in the second column are the same cases in first column with different time. (A) First mode quantized field; (B) First mode quantized field; (C) Second mode quantized field; (D) Second mode quantized field; (E) First mode quantized field; (F) First mode quantized field; (G) Second mode quantized field; (H) Second mode quantized field.

Figure 6. The Husimi function Q for the asymmetric two atoms (g = 0.5) at δ=0, λ=1 with γ=x+iy=5 and η=X+iY; first row represents M1=M2=0, second row for M1=M2=60, third row for M1=60 and M2=0, and the fourth row for M1=0 and M2=60; while the columns represent given moments. The first column for T = 0, second column for T = 12.5, third column for T = 20 and the fourth column T = 324.

Figure 6. The Husimi function Q for the asymmetric two atoms (g = 0.5) at δ=0, λ=1 with γ=x+iy=5 and η=X+iY; first row represents M1=M2=0, second row for M1=M2=60, third row for M1=60 and M2=0, and the fourth row for M1=0 and M2=60; while the columns represent given moments. The first column for T = 0, second column for T = 12.5, third column for T = 20 and the fourth column T = 324.