Here's a thinking process to determine the decay time for the 3p-1s transition in hydrogen:
- Understand the Request: The user wants the decay time (or lifetime) for a specific electron transition in a hydrogen atom: from the 3p state to the 1s state. They emphasize certainty and the use of calculations, suggesting a quantitative approach is needed.
- Identify Key Concepts:
- Electron Transition: An electron moving from a higher energy level (n=3, l=1) to a lower energy level (n=1, l=0).
- Decay Time / Lifetime (τ): The average time an atom stays in an excited state before decaying to a lower state via spontaneous emission.
- Spontaneous Emission: The process by which an excited atom emits a photon and transitions to a lower energy state without external stimulation.
- Transition Rate (A_if or Γ_if): The probability per unit time that an atom in initial state i will decay to final state f. The lifetime τ is the reciprocal of the total transition rate out of the initial state.
- Selection Rules: Not all transitions are allowed. For electric dipole transitions (the most common type), the change in the principal quantum number (Δn) can be anything, the change in the orbital angular momentum quantum number (Δl) must be ±1, and the change in the magnetic quantum number (Δm_l) must be 0 or ±1.
- Hydrogen Atom: The simplest atom, for which energy levels and wavefunctions are known exactly (within non-relativistic quantum mechanics).
- Check the Specific Transition:
- Initial state: n=3, l=1 (3p)
- Final state: n=1, l=0 (1s)
- Δn = 1 - 3 = -2 (allowed)
- Δl = 0 - 1 = -1 (allowed by electric dipole selection rules)
- Therefore, the 3p -> 1s transition is an allowed electric dipole transition.
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Determine the Calculation Needed: The decay time (lifetime, τ) of the initial state (3p) is requested. However, the lifetime of a state depends on all possible decay channels out of that state. The user asked specifically about the 3p -> 1s transition. This could mean either:
- The partial decay rate (or inverse lifetime) associated with only this specific transition.
- The total lifetime of the 3p state, considering all possible decays.
Let's re-read the question: "What is the decay time for the 3p-1s transition..." This phrasing is slightly ambiguous. It most likely refers to the partial lifetime associated with this specific decay channel, i.e., 1/A(3p1s). However, physicists often talk about the lifetime of the initial state. Let's clarify this. The lifetime τ of the 3p state is given by:
1/τ(3p) = A_total = A(3p1s) + A(3p2s) + A(3p3s) [Not possible] + ... Possible decays from 3p (n=3, l=1):- To n=1: Δl = 0 - 1 = -1. Allowed state is 1s. Transition: 3p -> 1s.
- To n=2: Δl can be ±1.
- l=0 (2s): Δl = 0 - 1 = -1. Allowed. Transition: 3p -> 2s.
- l=1 (2p): Δl = 1 - 1 = 0. Forbidden by electric dipole rules.
- l=2 (2d): Not possible for n=2.
- To n=3: l=0 (3s): Δl = 0-1 = -1. Allowed. Transition 3p -> 3s. (Though this is less common to consider spontaneously if energy difference is small/zero, standard formulas include it). Wait, 3p to 3s is allowed by selection rules, but the energy difference is zero (in simple models) or very small (fine structure). Spontaneous emission rate depends strongly on frequency cubed (ω³), so this rate would be negligible compared to others. Let's ignore decays within the same n shell for lifetime calculations unless specifically asked about fine structure effects.
So, the total decay rate from 3p is approximately A_total ≈ A(3p1s) + A(3p2s). The lifetime of the 3p state is τ(3p) = 1 / [A(3p1s) + A(3p2s)].
The question asks for the "decay time for the 3p-1s transition". This is most naturally interpreted as the partial lifetime τ_partial = 1 / A(3p->1s). However, it's crucial to state what is being calculated. It's better to calculate the total lifetime of the 3p state, as that's a more standard physical quantity, and mention the partial rates.
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Find the Formula for Transition Rate (Einstein A coefficient):
The spontaneous emission rate A_if for an electric dipole transition from initial state |i> = |n, l, m> to final state |f> = |n', l', m'> is given by:
A_if = (4 * α * ω_if³)/(3 * c²) * |<f| r |i>|²
where:- α is the fine-structure constant (≈ 1/137)
- ω_if is the angular frequency of the emitted photon (E_i - E_f) / ħ
- c is the speed of light
- r is the position operator (e * r is the dipole operator)
- <f| r |i> is the matrix element of the position operator between the initial and final states.
Often, the rate is averaged over initial m states and summed over final m' states (if degenerate). The formula often simplifies using the dipole matrix element squared, summed/averaged:
A(n,l -> n',l') = (4 * α * ω³)/(3 * c²) * (1/(2l+1)) * Σ_{m, m'} |<n', l', m'| r |n, l, m>|²This matrix element involves integrating the product of the final state wavefunction, the position operator (r * sinθ * cosφ, r * sinθ * sinφ, r * cosθ), and the initial state wavefunction over all space. The calculation involves radial integrals and angular integrals (using spherical harmonics).
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Locate Required Values/Perform Calculation:
- Energy Levels: E_n = -E_R / n², where E_R ≈ 13.6 eV is the Rydberg energy.
- E_3 = -13.6 / 9 eV
- E_1 = -13.6 / 1 eV
- E_2 = -13.6 / 4 eV
- Frequencies:
- ω(3p->1s) = (E_3 - E_1) / ħ = [-13.6/9 - (-13.6/1)] * e / ħ = (13.6 * 8/9) * e / ħ
- ω(3p->2s) = (E_3 - E_2) / ħ = [-13.6/9 - (-13.6/4)] * e / ħ = (13.6 * (1/4 - 1/9)) * e / ħ = (13.6 * 5/36) * e / ħ
- Matrix Elements: These are complex to calculate from scratch. They involve radial integrals with Laguerre polynomials and angular integrals with spherical harmonics. The result is often expressed in terms of the Bohr radius, a₀.
- |<1s| r |3p>|² (summed/averaged)
- |<2s| r |3p>|² (summed/averaged)
- Constants: α, c, ħ, e, a₀.
Calculating these matrix elements accurately is tedious and prone to errors. It's standard practice to look up these values from reliable physics sources (textbooks, databases).
- Energy Levels: E_n = -E_R / n², where E_R ≈ 13.6 eV is the Rydberg energy.
- Search for Pre-calculated Values: Search for "Einstein A coefficients hydrogen", "hydrogen 3p lifetime", "hydrogen transition probabilities 3p".
- NIST Atomic Spectra Database (ASD) is a highly reliable source. Searching there for H I lines.
- Textbooks like Bethe & Salpeter ("Quantum Mechanics of One- and Two-Electron Atoms") or Bransden & Joachain ("Physics of Atoms and Molecules") often list these values or formulas.
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Consult NIST ASD:
- Go to the NIST ASD Lines form.
- Enter "H I" as the spectrum.
- Set wavelength limits or energy levels to narrow down the search (e.g., lower level n=1, upper level n=3).
- Look for transitions originating from 3p (which might be listed as configuration 3p¹).
- Find the A_ki values (Einstein A coefficient) for transitions from 3p.
Searching NIST ASD for H I lines...
- Filter for lines where the upper level has configuration
3p
. - Transition 3p ¹P°₁ → 1s ¹S₀ (This notation includes term symbols and J values, which are relevant when considering fine structure, but for basic calculation 3p -> 1s is sufficient).
- Wavelength (Air): ~1025.7 Å (Lyman-beta)
- A_ki: 1.6725e+8 s⁻¹ (This is A(3p->1s))
- Transition 3p ¹P°₁ → 2s ¹S₀
- Wavelength (Air): ~6562.8 Å (H-alpha - Note: H-alpha is usually considered 3d2p, 3p2s, 3s2p combined, but NIST lists components) Let's re-check. Ah, H-alpha involves n=3 n=2. The strongest component is 3d2p. 3p2s is also part of it. Okay, NIST lists levels more precisely. Let's search by levels instead of lines.
- Go to NIST ASD Levels form.
- Search for H I, Energy Units eV.
- Find the level corresponding to 3p (Should be around E = -13.6/9 ≈ -1.51 eV relative to ionization limit, or 12.09 eV above ground state).
- Level: 12.0888 eV, Configuration: 3p, Term: ²P°
- There are two fine structure levels: J=1/2 and J=3/2. Their lifetimes might be slightly different. Let's look for the average or dominant value, or the rates from these levels.
- Go back to Lines form, inputting Upper Level Energy from 12.08 to 12.09 eV.
- Find lines originating from these 3p levels:
- Upper Level: 3p ²P° (J=1/2 or 3/2) -> Lower Level: 1s ²S₁/₂ (J=1/2)
- A_ki ≈ 1.67 x 10⁸ s⁻¹ (This is A(3p->1s))
- Upper Level: 3p ²P° (J=1/2 or 3/2) -> Lower Level: 2s ²S₁/₂ (J=1/2)
- A_ki ≈ 0.22 x 10⁸ s⁻¹ (This is A(3p->2s))
- Upper Level: 3p ²P° (J=1/2 or 3/2) -> Lower Level: 1s ²S₁/₂ (J=1/2)
- Calculate Lifetime:
- Total decay rate from 3p: A_total = A(3p1s) + A(3p2s)
- A_total ≈ (1.6725 x 10⁸ s⁻¹) + (0.2205 x 10⁸ s⁻¹) = 1.893 x 10⁸ s⁻¹
- Lifetime of the 3p state: τ(3p) = 1 / A_total = 1 / (1.893 x 10⁸ s⁻¹)
- Perform the Calculation (using Python):
Okay, let's determine the decay time associated with the 3p state of hydrogen, considering the 3p-1s transition.
- Understanding Decay Time: The "decay time" usually refers to the lifetime (τ) of the initial excited state (in this case, 3p). The lifetime is the average time the atom spends in the excited state before decaying to any lower energy state via spontaneous emission. It is the reciprocal of the total transition rate (total Einstein A coefficient, A_total) out of that state.
τ = 1 / A_total -
Identifying Possible Decay Channels: An electron in the 3p state (n=3, l=1) can decay to lower energy states provided the transition satisfies the electric dipole selection rules (Δl = ±1).
- Decay to n=1: The only state is 1s (n=1, l=0). Δl = 0 - 1 = -1. This transition (3p -> 1s) is allowed.
- Decay to n=2: Possible states are 2s (l=0) and 2p (l=1).
- 3p -> 2s: Δl = 0 - 1 = -1. This transition is allowed.
- 3p -> 2p: Δl = 1 - 1 = 0. This transition is forbidden by electric dipole rules (though allowed by weaker interactions, its rate is negligible here).
Therefore, the total decay rate from the 3p state is the sum of the rates for the allowed transitions:
A_total(3p) = A(3p 1s) + A(3p 2s) -
Finding the Transition Rates (Einstein A coefficients): These values are well-established and can be found in databases like the NIST Atomic Spectra Database (ASD).
- For the 3p 1s transition (Lyman-beta line): A(3p 1s) ≈ 1.6725 x 10⁸ s⁻¹
- For the 3p 2s transition: A(3p 2s) ≈ 0.2205 x 10⁸ s⁻¹
(Source: NIST ASD, querying transitions from H I level 3p)
- Calculating the Total Decay Rate and Lifetime:
We can now calculate the total decay rate and the lifetime of the 3p state using the values above.