This document describes a numerical renormalization group (NRG) computation of nuclear magnetic relaxation rates using a two-center basis approach. The NRG and Lanczos methods are used to calculate the spin-lattice relaxation rate 1/T1 as a function of temperature T and distance r from the impurity. Results show that 1/T1 dependence on T changes as the probe crosses the Kondo screening cloud radius rK, and the phase of low-energy Friedel oscillations also changes, indicating the Kondo screening cloud radius can be measured via NMR.
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Numerical Renormalization Group computation of magnetic relaxation rates
1. Numerical Renormalization-Group computation
of magnetic relaxation rates
Krissia de Zawadzki, Luiz Nunes de Oliveira, Jose Wilson M. Pinto
Instituto de F´ısica de S˜ao Carlos - Universidade de S˜ao Paulo
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 1 / 11
2. Introduction NRG calculations Numerical results Conclusions Acknowledgment
Radius of Kondo screening cloud
Radius of Kondo screening cloud
푅푘
LASZLO, B. PRB, 75 (2007). BOYCE, J.B; SLICHTER, C.P. PRL, 32, 61 (1974).
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 2 / 11
3. Introduction NRG calculations Numerical results Conclusions Acknowledgment
Radius of Kondo screening cloud
Radius of Kondo screening cloud
푅푘
푅퐾 ∝ 푇−1
퐾
General consensus
푅퐾 = ~푣퐹 /푘퐵푇퐾
Boyce
Slichter
NMR:
LASZLO, B. PRB, 75 (2007). BOYCE, J.B; SLICHTER, C.P. PRL, 32, 61 (1974).
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 2 / 11
4. Introduction NRG calculations Numerical results Conclusions Acknowledgment
Radius of Kondo screening cloud
Radius of Kondo screening cloud
푅푘
푅퐾 ∝ 푇−1
퐾
General consensus
푅퐾 = ~푣퐹 /푘퐵푇퐾
Boyce
Slichter
NMR:
LASZLO, B. PRB, 75 (2007). BOYCE, J.B; SLICHTER, C.P. PRL, 32, 61 (1974).
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 2 / 11
5. Introduction NRG calculations Numerical results Conclusions Acknowledgment
Radius of Kondo screening cloud
Radius of Kondo screening cloud
푅푘
푅퐾 ∝ 푇−1
퐾
General consensus
푅퐾 = ~푣퐹 /푘퐵푇퐾
Boyce
Slichter
NMR:
Experimental arrangement:
NMR probe: 푅 from the impurity
NRG computation of the spin
lattice relaxation rate 1/(푇1푇) as
function of 푇 and 푅
LASZLO, B. PRB, 75 (2007). BOYCE, J.B; SLICHTER, C.P. PRL, 32, 61 (1974).
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 2 / 11
6. Introduction NRG calculations Numerical results Conclusions Acknowledgment
Radius of Kondo screening cloud
Radius of Kondo screening cloud
푅푘
푅퐾 ∝ 푇−1
퐾
General consensus
푅퐾 = ~푣퐹 /푘퐵푇퐾
Boyce
Slichter
NMR:
Experimental arrangement:
NMR probe: 푅 from the impurity
NRG computation of the spin
lattice relaxation rate 1/(푇1푇) as
function of 푇 and 푅
Can we measure 푅퐾 via NMR?
Our
7. ndings:
Yes, we can!
T dependence changes as probe
crosses 푅퐾
Phase of low-푇 Friedel oscillations
also changes
LASZLO, B. PRB, 75 (2007). BOYCE, J.B; SLICHTER, C.P. PRL, 32, 61 (1974).
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 2 / 11
8. Introduction NRG calculations Numerical results Conclusions Acknowledgment
The quantum system
NRG Probe
Single-impurity Anderson model
퐻 =
퐻푐표푛푑 ⏞Σ︁ ⏟
k
휀k푐†
k푐k
휀 = 푣퐹
퐷 (푘 − 푘퐹 )
+퐷
−퐷
푘퐹
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 3 / 11
9. Introduction NRG calculations Numerical results Conclusions Acknowledgment
The quantum system
NRG Probe
Single-impurity Anderson model
퐻 =
퐻푐표푛푑 ⏞Σ︁ ⏟
k
휀k푐†
k푐k +
퐻푑 ⏞ ⏟
휀푑푐†
푑푐푑 + 푈푛푑↑푛푑↓
휀 = 푣퐹
퐷 (푘 − 푘퐹 )
+퐷
−퐷
푘퐹
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 3 / 11
10. Introduction NRG calculations Numerical results Conclusions Acknowledgment
The quantum system
NRG Probe
Single-impurity Anderson model
퐻 =
퐻푐표푛푑 ⏞Σ︁ ⏟
k
휀k푐†
k푐k +
퐻푑 ⏞ ⏟
휀푑푐†
푑푐푑 + 푈푛푑↑푛푑↓ +
퐻푖푛푡 ⏞√︂ ⏟
Γ
휋
(푓†
0 푐푑 + 퐻.푐.)
휀 = 푣퐹
퐷 (푘 − 푘퐹 )
+퐷
−퐷
푘퐹
푓0 =
1
√
휌
Σ︁
k
푐k
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 3 / 11
11. Introduction NRG calculations Numerical results Conclusions Acknowledgment
The quantum system
NRG Probe
Single-impurity Anderson model
퐻 =
퐻푐표푛푑 ⏞Σ︁ ⏟
k
휀k푐†
k푐k +
퐻푑 ⏞ ⏟
휀푑푐†
푑푐푑 + 푈푛푑↑푛푑↓ +
퐻푖푛푡 ⏞√︂ ⏟
Γ
휋
(푓†
0 푐푑 + 퐻.푐.)
퐻푝푟표푏푒 = −퐴
[︁
Ψ†
↑(⃗푅
)Ψ↓(⃗푅)퐼− + 퐻.푐.
]︁
Ψ휇 =
Σ︁
k
푒푖k.R푐k
1
푇1
=
4휋
~
Σ︁
퐼,퐹
푒−훽퐸퐼 |⟨퐼|퐻푝푟표푏푒|퐹⟩|2훿(퐸퐼 − 퐸퐹 )
푓0 =
1
√
휌
Σ︁
k
푐k
푅
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 3 / 11
12. Introduction NRG calculations Numerical results Conclusions Acknowledgment
Two-center basis
Two-center basis
Spherically symmetric operators
푐휀 =
Σ︁
k
푐 k 훿(휀 − 휀k) (around impurity)
푑휀 =
Σ︁
k
푐 k 푒푖k.R훿(휀 − 휀k) (around probe)
푐휀
푑휀
Zawadzki, K. de; Oliveira, L.N.; Pinto, J.W.M. NRG computation of nuclear magnetic relaxation rates 4 / 11