79 research outputs found
Many-body localization characterized from a one-particle perspective
We show that the one-particle density matrix can be used to
characterize the interaction-driven many-body localization transition in closed
fermionic systems. The natural orbitals (the eigenstates of ) are
localized in the many-body localized phase and spread out when one enters the
delocalized phase, while the occupation spectrum (the set of eigenvalues of
) reveals the distinctive Fock-space structure of the many-body
eigenstates, exhibiting a step-like discontinuity in the localized phase. The
associated one-particle occupation entropy is small in the localized phase and
large in the delocalized phase, with diverging fluctuations at the transition.
We analyze the inverse participation ratio of the natural orbitals and find
that it is independent of system size in the localized phase.Comment: 5 pages, 3 figures; v2: added two appendices and a new figure panel
in main text; v3: updated figur
A Deployment Process for Strategic Measurement Systems
Explicitly linking software-related activities to an organisation's
higher-level goals has been shown to be critical for organizational success.
GQM+Strategies provides mechanisms for explicitly linking goals and strategies,
based on goal-oriented strategic measurement systems. Deploying such strategic
measurement systems in an organization is highly challenging. Experience has
shown that a clear deployment strategy is needed for achieving sustainable
success. In particular, an adequate deployment process as well as corresponding
tool support can facilitate the deployment. This paper introduces the
systematical GQM+Strategies deployment process and gives an overview of
GQM+Strategies modelling and associated tool support. Additionally, it provides
an overview of industrial applications and describes success factors and
benefits for the usage of GQM+Strategies.Comment: 12 pages. Proceedings of the 8th Software Measurement European Forum
(SMEF 2011
ΠΠ΅ΡΡΠΎΡΡΡΡΠΊΡΡΡΠ½Π°Ρ ΡΠΈΠΏΠΈΠ·Π°ΡΠΈΡ ΡΠ»ΡΡΡΠ°ΠΌΠ°ΡΠΈΡΠΎΠ² ΠΠ°Π½ΡΠΊΠΎΠ³ΠΎ Π·Π΅Π»Π΅Π½ΠΎΠΊΠ°ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΏΠΎΡΡΠ° (ΡΠ΅Π²Π΅ΡΠΎ-Π·Π°ΠΏΠ°Π΄ ΠΠΎΡΡΠΎΡΠ½ΠΎΠ³ΠΎ Π‘Π°ΡΠ½Π°)
Π ΠΠ°Π½ΡΠΊΠΎΠΌ Π·Π΅Π»Π΅Π½ΠΎΠΊΠ°ΠΌΠ΅Π½Π½ΠΎΠΌ ΠΏΠΎΡΡΠ΅ (Π‘Π ΠΠΎΡΡΠΎΡΠ½ΠΎΠ³ΠΎ Π‘Π°ΡΠ½Π°) ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ Π΄Π²Π° ΡΠΈΠΏΠ° ΡΠ»ΡΡΡΠ°ΠΌΠ°ΡΠΈΡΠΎΠ²: ΠΌΠ°Π³ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π΄ΡΠ½ΠΈΡ-Π²Π΅ΡΠ»ΠΈΡ-ΠΏΠΈΠΊΡΠΈΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠΎΡΡΠ°Π²Π° ΠΈ ΡΠ΅ΡΡΠΈΡΠΎΠ²ΡΠ΅ Π΄ΡΠ½ΠΈΡ-Π³Π°ΡΡΠ±ΡΡΠ³ΠΈΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠΎΡΡΠ°Π²Π°. ΠΠ½ΠΈ ΠΎΠ±ΡΠ΅Π΄ΠΈΠ½Π΅Π½Ρ Π² ΠΊΠΈΠ½Π³Π°ΡΡΠΊΠΈΠΉ ΠΈ ΠΈΠ΄Π°ΡΡΠΊΠΈΠΉ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΡ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½ΠΎ
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