1995
DOI: 10.1088/0305-4470/28/1/011
|View full text |Cite
|
Sign up to set email alerts
|

Local critical behaviour at aperiodic surface extended perturbation in the Ising quantum chain

Abstract: The surface critical behaviour of the semi-infinite one-dimensional quantum Ising model in a transverse field is studied in the presence of an aperiodic surface extended modulation. The perturbed couplings are distributed according to a generalized Fredholm sequence, leading to a marginal perturbation and varying surface exponents. The surface magnetic exponents are calculated exactly whereas the expression of the surface energy density exponent is conjectured from a finitesize scaling study. The system displa… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

0
26
0

Year Published

1995
1995
1999
1999

Publication Types

Select...
5

Relationship

1
4

Authors

Journals

citations
Cited by 11 publications
(26 citation statements)
references
References 39 publications
0
26
0
Order By: Relevance
“…In the last years, much progress have been made in the understanding of the properties of marginal and relevant aperiodically perturbed systems. Exact results for the 2D layered Ising model and the quantum Ising chain have been obtained with irrelevant, marginal and relevant aperiodic perturbations [29,30,31,32]. The critical behaviour is in agreement with Luck's criterion, leading to essential singularities or first-order surface transition when the perturbation is relevant and power laws with continuously varying exponents in the marginal situation with logarithmically diverging fluctuations.…”
Section: Introductionmentioning
confidence: 54%
“…In the last years, much progress have been made in the understanding of the properties of marginal and relevant aperiodically perturbed systems. Exact results for the 2D layered Ising model and the quantum Ising chain have been obtained with irrelevant, marginal and relevant aperiodic perturbations [29,30,31,32]. The critical behaviour is in agreement with Luck's criterion, leading to essential singularities or first-order surface transition when the perturbation is relevant and power laws with continuously varying exponents in the marginal situation with logarithmically diverging fluctuations.…”
Section: Introductionmentioning
confidence: 54%
“…The scaling dimension x s e of the surface energy can be deduced from the finite-size behaviour e s = 0|σ x 1 |ε where the state |ε = η † 1 η † 2 |0 is the lowest two-particle excitated state. This matrix element can be written as [19]:…”
Section: Discussionmentioning
confidence: 99%
“…x s e = 1 + 2β s (5.12) if one assumes that φ 2 (1) scale as L −βs too. This is known to be true either for the marginal HvL model [20] or for the aperiodic version of the same model [19] where the couplings are modulated according to the Fredholm sequence [17]. When the transition is first-order, due to the localization of φ 1 , the scaling of the first excitation is anomalous [21]:…”
Section: Discussionmentioning
confidence: 99%
“…This is known to be true either for the marginal HvL model [20] or for the aperiodic version of the same model [19] where the couplings are modulated according to the Fredholm sequence [17]. When the transition is first-order, due to the localization of φ 1 , the scaling of the first excitation is anomalous [21]:…”
Section: Discussionmentioning
confidence: 99%
“…Furthermore we assumed that, like in Refs. [19,20], φ 2 (1) scales as L −β ′ s /2 . As for the HvL model, in the regime of first-order transition, the anomalous scaling of the first gap leads to an exponent asymmetry [5].…”
Section: Discussionmentioning
confidence: 99%