43 research outputs found
Reconciling the interests of the economic diversification participants in a single-industry town
Π Π°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°ΡΡΡΡ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² ΡΡΠ°ΡΡΠ½ΠΈΠΊΠΎΠ² ΠΏΡΠΎΡΠ΅ΡΡΠ° Π΄ΠΈΠ²Π΅ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΠΊΠΈ ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π° Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ΠΌ ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π° Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΡΡΡΠ°ΡΠ΅Π³ΠΈΠΈ Π΄ΠΈΠ²Π΅ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ. Π¦Π΅Π»ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΈΠ½ΡΡΡΡΠΌΠ΅Π½ΡΠΎΠ² Π³Π°ΡΠΌΠΎΠ½ΠΈΠ·Π°ΡΠΈΠΈ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² ΡΡΠ°ΡΡΠ½ΠΈΠΊΠΎΠ² ΠΏΡΠΎΡΠ΅ΡΡΠ° Π΄ΠΈΠ²Π΅ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΠΊΠΈ ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π° Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² ΠΈ ΡΠΎΠΏΠΎΡΡΠ°Π²Π»Π΅Π½ΠΈΡ Π΅Π΅ Ρ ΠΌΠΎΠ΄Π΅Π»ΡΡ ΠΎΡΠ΄Π΅Π»ΡΠ½ΠΎ Π²Π·ΡΡΠΎΠ³ΠΎ ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π°. ΠΠ΅ΡΠΎΠ΄Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ: ΡΠΈΡΡΠ΅ΠΌΠ½ΡΠΉ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄, Π°Π½Π°Π»ΠΈΠ· ΠΈ ΡΠΈΠ½ΡΠ΅Π·, ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΠ΅ ΠΌΠ½ΠΎΠΆΠ΅ΡΡΠ² ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π΄ΠΈΠ°Π³ΡΠ°ΠΌΠΌΡ ΠΠΉΠ»Π΅ΡΠ°-ΠΠ΅Π½Π½Π°, ΠΌΠ΅ΡΠΎΠ΄Ρ ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΎΡΠΈΠΊΠΈ, ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΠ΅ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΠΈ ΡΡΠ΄ΠΎΠ² Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ, Π³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΈ ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΡ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΠΈ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ². Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π° ΠΌΠΎΠ΄Π΅Π»Ρ ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π³ΡΡΠΏΠΏ Π»ΠΈΡ, Π² ΠΊΠΎΡΠΎΡΠΎΠΉ ΠΎΡΡΠ°ΠΆΠ΅Π½Ρ ΡΡΠ΅ΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΠ³ΠΎ ΠΏΠ΅ΡΠ΅ΡΠ΅ΡΠ΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ², Π° ΡΠ°ΠΊΠΆΠ΅ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΡ ΡΠΈΡΠ»Π° ΡΠΎΠ³Π»Π°ΡΡΠ΅ΠΌΡΡ
ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ². ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ ΠΎΡΠ½ΠΎΠ²Π½ΡΠ΅ Π³ΡΡΠΏΠΏΡ ΡΡΠ°ΡΡΠ½ΠΈΠΊΠΎΠ² ΠΏΡΠΎΡΠ΅ΡΡΠ° Π΄ΠΈΠ²Π΅ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π°, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠ°Π·Π³ΡΠ°Π½ΠΈΡΠ΅Π½ΠΎ ΠΏΠΎΠ½ΡΡΠΈΠ΅ ΡΡΠ°ΡΡΠ½ΠΈΠΊΠ° ΠΈ ΡΠΎΠ»ΠΈ (ΡΡΠ½ΠΊΡΠΈΠΈ) ΡΡΠ°ΡΡΠ½ΠΈΠΊΠ° Π² Π΄Π°Π½Π½ΠΎΠΌ ΠΏΡΠΎΡΠ΅ΡΡΠ΅. ΠΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΎ ΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΎ ΡΠΈΡΠ»ΠΎ ΠΌΠ½ΠΎΠΆΠ΅ΡΡΠ² Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΠΈΡΠ»Π° ΡΡΠ°ΡΡΠ½ΠΈΠΊΠΎΠ², ΡΡΠΈ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΡ ΠΎΠ΄Π½ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎ ΡΠΎΠ³Π»Π°ΡΡΡΡΡΡ, Π½Π° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π° ΠΠ°Π»ΡΠ°Π½ ΠΠ΅ΠΌΠ΅ΡΠΎΠ²ΡΠΊΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΏΠΎΡΡΡΠΎΠ΅Π½Π° ΠΌΠΎΠ΄Π΅Π»Ρ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² Π½Π° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π° ΠΠ°Π»ΡΠ°Π½Π°. ΠΠΎΠ»ΡΡΠ΅Π½Π½Π°Ρ ΠΌΠΎΠ΄Π΅Π»Ρ ΠΈΠΌΠ΅Π΅Ρ ΡΡΠ°ΠΏΠ΅ΡΠΈΠ΅Π²ΠΈΠ΄Π½ΡΡ ΡΠΎΡΠΌΡ, ΡΡΠΎ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΠ΅Ρ ΠΎ Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎ Π½Π΅Π±ΠΎΠ»ΡΡΠΎΠΌ ΡΠΈΡΠ»Π΅ ΠΎΠ±ΡΠΈΡ
ΡΠΎΠ³Π»Π°ΡΡΠ΅ΠΌΡΡ
ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ². ΠΠ²ΡΠΎΡ ΠΏΡΠΈΡ
ΠΎΠ΄ΠΈΡ ΠΊ Π²ΡΠ²ΠΎΠ΄Ρ, ΡΡΠΎ Π² ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π΅ ΡΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ ΡΡΠ΅ΡΠ³ΠΎΠ»ΡΠ½ΠΈΠΊ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² Β«Π°Π΄ΠΌΠΈΠ½ΠΈΡΡΡΠ°ΡΠΈΡ Π³ΠΎΡΠΎΠ΄Π° - ΠΌΠ°Π»ΡΠΉ Π±ΠΈΠ·Π½Π΅Ρ Π² ΡΠΎΠ»ΠΈ ΠΈΠ½Π²Π΅ΡΡΠΎΡΠ° - Π²ΡΠ·Β», ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡΠΈΠΉ ΠΎΡΠ½ΠΎΠ²Ρ Π² ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΠΈ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π° ΠΠ°Π»ΡΠ°Π½. Π¦Π΅Π½ΡΡΠ°Π»ΡΠ½ΠΎΠ΅ ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠ΅ ΠΏΡΠΈ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² Ρ ΠΏΡΠΎΡΠΈΠΌΠΈ ΡΡΠ°ΡΡΠ½ΠΈΠΊΠ°ΠΌΠΈ Π·Π°Π½ΠΈΠΌΠ°Π΅Ρ ΠΈΡΠΊΠ»ΡΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π°Π΄ΠΌΠΈΠ½ΠΈΡΡΡΠ°ΡΠΈΡ Π³ΠΎΡΠΎΠ΄Π°. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ Π΄Π°Π½Π½ΡΡ
Π²ΡΠ²ΠΎΠ΄ΠΎΠ² Π²Π½Π΅ΡΠ΅Π½Ρ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ΠΈΡ ΠΏΠΎ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡΠΌ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅Π³ΠΎ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠΎΠ² Π½Π° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΠΌΠΎΠ³ΠΎ ΠΌΠΎΠ½ΠΎΠ³ΠΎΡΠΎΠ΄Π°.The article explores the problems of reconciling the interests of single-industry towns, a need that arises from the entire process of industry development management through a diversification strategy. The aim of this study is to develop tools to harmonize the interests of the single-industry towns, based on a model of full harmonization with the model of an individual single-industry town. Methods of the research: system approach, analysis and synthesis, building a set of harmonized interests with the application of the Eulerian-Venn diagram, combinatorics methods, construction of economic indicators and series of dynamics, graphical method of presentation of results and building the hierarchy of interests. Results of the study. The paper introduces the model for fully reconciling the interests of different groups of persons, reflecting the areas of possible intersecting interests and the hierarchy of the number of interests involved. The article proposes the main groups of participants in the diversification process and the differentially concept of participant and the role (function) of the participant in the diversification process. The author justifies and estimates the number of sets depending on the number of participants whose interests are concurrently reconciled in Kaltan case study. The proposed model is used for Kaltan, Kemerovo region case study. The result ing model is of a trapezoidal form, which indicates that there are quite a few common consenting interests. The author concludes that a triangle of interests Β«city administration - small business as investor - universityΒ» is formed. This triangle represents the highest level of harmonization of interests in the hierarchy. The city administration is in central position in reconciling interests with other participants. By the example of the considered single-industry town and based on these findings the suggestion on further harmonization of interests was made
Evidence for even parity unconventional superconductivity in Sr2RuO4
Funding:Β A.C. is grateful for support from the Julian Schwinger Foundation for Physics Research. A.P. acknowledges support by the Alexander von Humboldt Foundation through the Feodor Lynen Fellowship. Work at Los Alamos was funded by Laboratory Directed Research and Development (LDRD) program, and A.P. acknowledges partial support through the LDRD. N.K. acknowledges the support by the Grants-in-Aid for Scientific Research (KAKENHI, Grant JP18K04715 and JP21H01033) from Japan Society for the Promotion of Science (JSPS). The work at Dresden was funded by the Deutsche Forschungsgemeinschaft - TRR 288 - 422213477 (projects A10 and B01). The work at University of California, Los Angeles, was supported by NSF Grants 1709304 and 2004553.Unambiguous identification of the superconducting order parameter symmetry in Sr2RuO4Β has remained elusive for more than a quarter century. While a chiral p-wave ground state analogue to superfluid 3He-A was ruled out only very recently, other proposed triplet-pairing scenarios are still viable. Establishing the condensate magnetic susceptibility reveals a sharp distinction between even-parity (singlet) and odd-parity (triplet) pairing since the superconducting condensate is magnetically polarizable only in the latter case. Here field-dependent 17O Knight shift measurements, being sensitive to the spin polarization, are compared to previously reported specific heat measurements for the purpose of distinguishing the condensate contribution from that due to quasiparticles. We conclude that the shift results can be accounted for entirely by the expected field-induced quasiparticle response. An upper bound for the condensate magnetic response of < 10% of the normal state susceptibility is sufficient to exclude all purely odd-parity candidates.Β PostprintPeer reviewe
Thermodynamic Evidence for a Two-Component Superconducting Order Parameter in SrRuO
SrRuO has stood as the leading candidate for a spin-triplet
superconductor for 26 years. Recent NMR experiments have cast doubt on this
candidacy, however, and it is difficult to find a theory of superconductivity
that is consistent with all experiments. What is needed are symmetry-based
experiments that can rule out broad classes of possible superconducting order
parameters. Here we use resonant ultrasound spectroscopy to measure the entire
symmetry-resolved elastic tensor of SrRuO through the superconducting
transition. We observe a thermodynamic discontinuity in the shear elastic
modulus , requiring that the superconducting order parameter is
two-component. A two-component -wave order parameter, such as ,
naturally satisfies this requirement. As this order parameter appears to be
precluded by recent NMR experiments, we suggest that two other two-component
order parameters, namely or
, are now the prime candidates for
the order parameter of SrRuO
High sensitivity heat capacity measurements on Sr2RuO4 under uniaxial pressure
Funding: Parts of this work were funded by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) - TRR 288 -422213477 (projects A10 and B01). NK acknowledges the support from JSPS KAKENHI (nos. JP17H06136 and JP18K04715) and JST-Mirai Program (no. JPMJMI18A3) in Japan and YM from JSPS KAKENHI (nos. JP15H05852, JP15K21717) and JSPS core-to-core programme. YSL acknowledges the support of a St Leonardβs scholarship from the University of St Andrews, the Engineering and Physical Sciences Research Council via the Scottish Condensed Matter Centre for Doctoral Training under grant EP/G03673X/1, and the Max Planck Society.A key question regarding the unconventional superconductivity of Sr2RuO4 remains whether the order parameter is single- or two-component. Under a hypothesis of two-component superconductivity, uniaxial pressure is expected to lift their degeneracy, resulting in a split transition. The most direct and fundamental probe of a split transition is heat capacity. Here, we report development of new high-frequency methodology for measurement of heat capacity of samples subject to large and highly homogeneous uniaxial pressure. We place an upper limit on the heat capacity signature of any second transition of a few per cent of the primary superconducting transition. The normalized jump in heat capacity, Ξ C/C, grows smoothly as a function of uniaxial pressure, but we find no qualitative evidence of a pressure-induced order parameter transition. Thanks to the high precision of our measurements, these findings place stringent constraints on theories of the superconductivity of Sr2RuO4.PostprintPeer reviewe
Strong peak in Tc of Sr2RuO4Β under uniaxial pressure
Sr2RuO4 is an unconventional superconductor that has attracted widespread study because of its high purity and the possibility that its superconducting order parameter has odd parity. We study the dependence of its superconductivity on anisotropic strain. Applying uniaxial pressures of up to ~1 gigapascals along a γ100γ direction (a axis) of the crystal lattice results in the transition temperature (Tc) increasing from 1.5 kelvin in the unstrained material to 3.4 kelvin at compression by β0.6%, and then falling steeply. Calculations give evidence that the observed maximum Tc occurs at or near a Lifshitz transition when the Fermi level passes through a Van Hove singularity, and open the possibility that the highly strained, Tc = 3.4 K Sr2RuO4 has an even-parity, rather than an odd-parity, order parameter.PostprintPeer reviewe
Elastocaloric determination of the phase diagram of SrRuO
One of the main developments in unconventional superconductivity in the past two decades has been the discovery that most unconventional superconductors form phase diagrams that also contain other strongly correlated states. Many systems of interest are therefore close to more than one instability, and tuning between the resultant ordered phases is the subject of intense research1. In recent years, uniaxial pressure applied using piezoelectric-based devices has been shown to be a particularly versatile new method of tuning, leading to experiments that have advanced our understanding of the fascinating unconventional superconductor SrRuO. Here we map out its phase diagram using high-precision measurements of the elastocaloric effect in what we believe to be the first such study including both the normal and the superconducting states. We observe a strong entropy quench on entering the superconducting state, in excellent agreement with a model calculation for pairing at the Van Hove point, and obtain a quantitative estimate of the entropy change associated with entry to a magnetic state that is observed in proximity to the superconductivity. The phase diagram is intriguing both for its similarity to those seen in other families of unconventional superconductors and for extra features unique, so far, to SrRuO
Upper Critical Field of SrRuO under In-Plane Uniaxial Pressure
In-plane uniaxial pressure has been shown to strongly tune the
superconducting state of SrRuO by approaching a Lifshitz transition and
associated Van Hove singularity (VHS) in the density of states. At the VHS,
and the in- and out-of-plane upper critical fields are all strongly
enhanced, and the latter has changed its curvature as a function of temperature
from convex to concave. However, due to strain inhomogeneity it has not been
possible so far to determine how the upper critical fields change with strain.
Here, we show the strain dependence of both upper critical fields, which was
achieved due to an improved sample preparation. We find that the in-plane upper
critical field is mostly linear in . On the other hand, the out-of-plane
upper critical field varies with a higher power in , and peaks strongly at
the VHS. The strong increase in magnitude and the change in form of
occur very close to the Van Hove strain, and points to a
strong enhancement of both the density of states and the gap magnitude at the
Lifshitz transition
Kazalo
The superconducting state in the quasi-two-dimensional and strongly
correlated SrRuO is uniquely held up as a solid state analog to
superfluid He-, with an odd-parity order parameter that also breaks time
reversal symmetry, and for which the vector order parameter has the same
direction in spin space for all electron momenta. The recent discovery that
uniaxial pressure causes a steep rise and maximum in transition temperature
() in strained samples motivated the study of O nuclear magnetic
resonance (NMR) that we describe in this article. A reduction of Knight shifts
was observed for all strain values and temperatures , consistent
with a drop in spin polarization in the superconducting state. In unstrained
samples, our results are in contradiction with a body of previous NMR work, and
with the most prominent previous proposals for the order parameter of
SrRuO. Possible alternative scenarios are discussed.Comment: Manuscript: 4 figures, 2 tables; Supplementary Information: 5 figure
Normal state 17O NMR studies of Sr2RuO4 under uniaxial stress
This work was supported in part by the Laboratory Directed Research and Development (LDRD) program of Los Alamos National Laboratory under Project No. 20170204ER. Y. L. acknowledges partial support through the LDRD and 1000 Youth Talents Plan of China. N. K. acknowledges the support from JSPS KAKNHI (Grant No. 18K04715). I. I.M. is supported by ONR through the NRL basic research program. This work is supported in part by the National Science Foundation (Grants No. DMR-1410343 and No. DMR-1709304).The effects of uniaxial compressive stress on the normal state 17O nuclear-magnetic-resonance properties of the unconventional superconductor Sr2RuO4 are reported. The paramagnetic shifts of both planar and apical oxygen sites show pronounced anomalies near the nominal a-axis strain Ο΅aaβ‘Ο΅v that maximizes the superconducting transition temperature Tc. The spin susceptibility weakly increases on lowering the temperature below Tβ10ββK, consistent with an enhanced density of states associated with passing the Fermi energy through a van Hove singularity. Although such a Lifshitz transition occurs in the Ξ³ band formed by the Ru dxy states hybridized with in-plane O pΟ orbitals, the large Hundβs coupling renormalizes the uniform spin susceptibility, which, in turn, affects the hyperfine fields of all nuclei. We estimate this βStonerβ renormalization S by combining the data with first-principles calculations and conclude that this is an important part of the strain effect, with implications for superconductivity.Publisher PDFPeer reviewe