Random walk in a high density dynamic random environment
The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibr...
Ausführliche Beschreibung
Autor*in: |
den Hollander, Frank [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2014transfer abstract |
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Umfang: |
15 |
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Übergeordnetes Werk: |
Enthalten in: Optical and white light emission properties of Dy - Babu, P. ELSEVIER, 2021, Amsterdam |
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Übergeordnetes Werk: |
volume:25 ; year:2014 ; number:4 ; day:27 ; month:06 ; pages:785-799 ; extent:15 |
Links: |
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DOI / URN: |
10.1016/j.indag.2014.04.010 |
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Katalog-ID: |
ELV039537668 |
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520 | |a The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. | ||
520 | |a The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. | ||
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10.1016/j.indag.2014.04.010 doi GBVA2014021000005.pica (DE-627)ELV039537668 (ELSEVIER)S0019-3577(14)00039-1 DE-627 ger DE-627 rakwb eng 510 510 DE-600 530 VZ 33.60 bkl 51.00 bkl den Hollander, Frank verfasserin aut Random walk in a high density dynamic random environment 2014transfer abstract 15 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. Dynamic random environment Elsevier Random walk Elsevier Law of large numbers Elsevier Multi-scale renormalization Elsevier Kesten, Harry oth Sidoravicius, Vladas oth Enthalten in Elsevier Babu, P. ELSEVIER Optical and white light emission properties of Dy 2021 Amsterdam (DE-627)ELV006009107 volume:25 year:2014 number:4 day:27 month:06 pages:785-799 extent:15 https://doi.org/10.1016/j.indag.2014.04.010 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 25 2014 4 27 0627 785-799 15 045F 510 |
spelling |
10.1016/j.indag.2014.04.010 doi GBVA2014021000005.pica (DE-627)ELV039537668 (ELSEVIER)S0019-3577(14)00039-1 DE-627 ger DE-627 rakwb eng 510 510 DE-600 530 VZ 33.60 bkl 51.00 bkl den Hollander, Frank verfasserin aut Random walk in a high density dynamic random environment 2014transfer abstract 15 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. Dynamic random environment Elsevier Random walk Elsevier Law of large numbers Elsevier Multi-scale renormalization Elsevier Kesten, Harry oth Sidoravicius, Vladas oth Enthalten in Elsevier Babu, P. ELSEVIER Optical and white light emission properties of Dy 2021 Amsterdam (DE-627)ELV006009107 volume:25 year:2014 number:4 day:27 month:06 pages:785-799 extent:15 https://doi.org/10.1016/j.indag.2014.04.010 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 25 2014 4 27 0627 785-799 15 045F 510 |
allfields_unstemmed |
10.1016/j.indag.2014.04.010 doi GBVA2014021000005.pica (DE-627)ELV039537668 (ELSEVIER)S0019-3577(14)00039-1 DE-627 ger DE-627 rakwb eng 510 510 DE-600 530 VZ 33.60 bkl 51.00 bkl den Hollander, Frank verfasserin aut Random walk in a high density dynamic random environment 2014transfer abstract 15 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. Dynamic random environment Elsevier Random walk Elsevier Law of large numbers Elsevier Multi-scale renormalization Elsevier Kesten, Harry oth Sidoravicius, Vladas oth Enthalten in Elsevier Babu, P. ELSEVIER Optical and white light emission properties of Dy 2021 Amsterdam (DE-627)ELV006009107 volume:25 year:2014 number:4 day:27 month:06 pages:785-799 extent:15 https://doi.org/10.1016/j.indag.2014.04.010 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 25 2014 4 27 0627 785-799 15 045F 510 |
allfieldsGer |
10.1016/j.indag.2014.04.010 doi GBVA2014021000005.pica (DE-627)ELV039537668 (ELSEVIER)S0019-3577(14)00039-1 DE-627 ger DE-627 rakwb eng 510 510 DE-600 530 VZ 33.60 bkl 51.00 bkl den Hollander, Frank verfasserin aut Random walk in a high density dynamic random environment 2014transfer abstract 15 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. Dynamic random environment Elsevier Random walk Elsevier Law of large numbers Elsevier Multi-scale renormalization Elsevier Kesten, Harry oth Sidoravicius, Vladas oth Enthalten in Elsevier Babu, P. ELSEVIER Optical and white light emission properties of Dy 2021 Amsterdam (DE-627)ELV006009107 volume:25 year:2014 number:4 day:27 month:06 pages:785-799 extent:15 https://doi.org/10.1016/j.indag.2014.04.010 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 25 2014 4 27 0627 785-799 15 045F 510 |
allfieldsSound |
10.1016/j.indag.2014.04.010 doi GBVA2014021000005.pica (DE-627)ELV039537668 (ELSEVIER)S0019-3577(14)00039-1 DE-627 ger DE-627 rakwb eng 510 510 DE-600 530 VZ 33.60 bkl 51.00 bkl den Hollander, Frank verfasserin aut Random walk in a high density dynamic random environment 2014transfer abstract 15 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. Dynamic random environment Elsevier Random walk Elsevier Law of large numbers Elsevier Multi-scale renormalization Elsevier Kesten, Harry oth Sidoravicius, Vladas oth Enthalten in Elsevier Babu, P. ELSEVIER Optical and white light emission properties of Dy 2021 Amsterdam (DE-627)ELV006009107 volume:25 year:2014 number:4 day:27 month:06 pages:785-799 extent:15 https://doi.org/10.1016/j.indag.2014.04.010 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 25 2014 4 27 0627 785-799 15 045F 510 |
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The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. |
abstractGer |
The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. |
abstract_unstemmed |
The goal of this note is to prove a law of large numbers for the empirical speed of a green particle that performs a random walk on top of a field of red particles which themselves perform independent simple random walks on Z d , d ≥ 1 . The red particles jump at rate 1 and are in a Poisson equilibrium with density μ . The green particle also jumps at rate 1, but uses different transition kernels p ′ and p ″ depending on whether it sees a red particle or not. It is shown that, in the limit as μ → ∞ , the speed of the green particle tends to the average jump under p ′ . This result is far from surprising, but it is non-trivial to prove. The proof that is given in this note is based on techniques that were developed in Kesten and Sidoravicius (2005) to deal with spread-of-infection models. The main difficulty is that, due to particle conservation, space–time correlations in the field of red particles decay slowly. This places the problem in a class of random walks in dynamic random environments for which scaling laws are hard to obtain. |
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