cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.137769.v1/t34
title: "Aux Figure 08c" of "Search for nonresonant pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: The observed 95% CL exclusion limits as a function of the five relevant SMEFT coefficients: (a) c<sub>H</sub>, (b) c<sub>H G</sub>, (c) c<sub>H□</sub>, (d) c<sub>tH</sub>, and (e) c<sub>tG</sub>, obtained from the combined ggF signal model, as shown by the solid black line.
The values of the other four coefficients are fixed to 0.
The blue and yellow bands show the 1σ and 2σ bands respectively on the expected exclusion limits, which are shown by the dashed black line.
The red line shows the predicted ggF HH cross-section as a function of the coefficient.
The VBF HH process is ignored for this result.
description: No data abstract available.
DOI: 10.17182/hepdata.137769.v1/t35
title: "Aux Figure 08d" of "Search for nonresonant pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: The observed 95% CL exclusion limits as a function of the five relevant SMEFT coefficients: (a) c<sub>H</sub>, (b) c<sub>H G</sub>, (c) c<sub>H□</sub>, (d) c<sub>tH</sub>, and (e) c<sub>tG</sub>, obtained from the combined ggF signal model, as shown by the solid black line.
The values of the other four coefficients are fixed to 0.
The blue and yellow bands show the 1σ and 2σ bands respectively on the expected exclusion limits, which are shown by the dashed black line.
The red line shows the predicted ggF HH cross-section as a function of the coefficient.
The VBF HH process is ignored for this result.
description: No data abstract available.
DOI: 10.17182/hepdata.137769.v1/t36
title: "Aux Figure 08e" of "Search for nonresonant pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: The observed 95% CL exclusion limits as a function of the five relevant SMEFT coefficients: (a) c<sub>H</sub>, (b) c<sub>H G</sub>, (c) c<sub>H□</sub>, (d) c<sub>tH</sub>, and (e) c<sub>tG</sub>, obtained from the combined ggF signal model, as shown by the solid black line.
The values of the other four coefficients are fixed to 0.
The blue and yellow bands show the 1σ and 2σ bands respectively on the expected exclusion limits, which are shown by the dashed black line.
The red line shows the predicted ggF HH cross-section as a function of the coefficient.
The VBF HH process is ignored for this result.
description: No data abstract available.
DOI: 10.17182/hepdata.137769.v1/t37
title: "Aux Figure 09a" of "Search for nonresonant pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: The observed 95% CL exclusion limits as a function of the two relevant HH HEFT coefficients: (a) c<sub>tt̄HH</sub> and (b) c<sub>ggHH</sub>, obtained from the combined ggF signal model, as shown by the solid black line.
The values of the other four coefficients are fixed to 0.
The blue and yellow bands show the 1σ and 2σ bands respectively on the expected exclusion limits, which are shown by the dashed black line.
The red line shows the predicted ggF HH cross-section as a function of the coefficient.
The VBF HH process is ignored for this result.
description: No data abstract available.
DOI: 10.17182/hepdata.137769.v1/t38
title: "Aux Figure 09b" of "Search for nonresonant pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: The observed 95% CL exclusion limits as a function of the two relevant HH HEFT coefficients: (a) c<sub>tt̄HH</sub> and (b) c<sub>ggHH</sub>, obtained from the combined ggF signal model, as shown by the solid black line.
The values of the other four coefficients are fixed to 0.
The blue and yellow bands show the 1σ and 2σ bands respectively on the expected exclusion limits, which are shown by the dashed black line.
The red line shows the predicted ggF HH cross-section as a function of the coefficient.
The VBF HH process is ignored for this result.
description: No data abstract available.
DOI: 10.17182/hepdata.137817.v1/t1
title: "T_2pi0(costh)" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetry for $\pi^0\pi^0$ as a function of the polar angle for bins of the incident photon energy in the range of $E_\gamma$ = 650-2600 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t2
title: "T_2pi0(m)" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetry for $\pi^0\pi^0$ as a function of the $\pi^0\pi^0$ invariant mass for bins of the incident photon energy in the range of $E_\gamma$ = 650-2600 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t3
title: "Pxy_2pi0(phi*)" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetry for $\pi^0\pi^0$ as a function of the $\phi^*$ angle for bins of the incident photon energy in the range of $E_\gamma$ = 650-2600 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t10
title: "PH_ppi0(m)" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $p\pi^0$ as a function of the $p\pi0$ invariant mass for bins of the incident photon energy in the range of $E_\gamma$ = 650-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t4
title: "T_ppi0(costh)" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetry for $p\pi^0$ as a function of the polar angle for bins of the incident photon energy in the range of $E_\gamma$ = 650-2600 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t5
title: "T_ppi0(m)" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetry for $p\pi^0$ as a function of the $p\pi0$ invariant mass for bins of the incident photon energy in the range of $E_\gamma$ = 650-2600 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t6
title: "Pxy_ppi0(phi*)" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetry for $p\pi^0$ as a function of the $\phi^*$ angle for bins of the incident photon energy in the range of $E_\gamma$ = 650-2600 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t7
title: "PH_2pi0(costh)" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $\pi^0\pi^0$ as a function of the polar angle for bins of the incident photon energy in the range of $E_\gamma$ = 650-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t8
title: "PH_2pi0(m)" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $\pi^0\pi^0$ as a function of the $\pi^0\pi0$ invariant mass for bins of the incident photon energy in the range of $E_\gamma$ = 650-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t11
title: "Pxysc_2pi0(phi*)" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $\pi^0\pi^0$ as a function of the $\phi^*$ angle for bins of the incident photon energy in the range of $E_\gamma$ = 650-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t12
title: "Pxysc_ppi0(phi*)" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $p\pi^0$ as a function of the $\phi^*$ angle for bins of the incident photon energy in the range of $E_\gamma$ = 650-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t13
title: "Pxy_2pi0(4D)_650MeV" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetries for $\pi^0\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 650-800 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t14
title: "Pxy_2pi0(4D)_800MeV" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetries for $\pi^0\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 800-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t15
title: "Pxy_2pi0(4D)_950MeV" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetries for $\pi^0\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 950-1100 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t16
title: "Pxy_2pi0(4D)_1100MeV" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetries for $\pi^0\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 1100-1250 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t9
title: "PH_ppi0(costh)" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $\pi^0\pi^0$ as a function of the polar angle for bins of the incident photon energy in the range of $E_\gamma$ = 650-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t17
title: "Pxy_ppi0(4D)_650MeV" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetries for $p\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 650-800 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t18
title: "Pxy_ppi0(4D)_800MeV" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetries for $p\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 800-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t19
title: "Pxy_ppi0(4D)_950MeV" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetries for $p\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 950-1100 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t20
title: "Pxy_ppi0(4D)_1100MeV" of "Polarization observables in double neutral pion photoproduction"

description: Target asymmetries for $p\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 1100-1250 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t21
title: "Pxysc_2pi0(4D)_650MeV" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $\pi^0\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 650-800 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t22
title: "Pxysc_2pi0(4D)_800MeV" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $\pi^0\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 800-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t23
title: "Pxysc_ppi0(4D)_650MeV" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $p\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 650-800 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137817.v1/t24
title: "Pxysc_ppi0(4D)_800MeV" of "Polarization observables in double neutral pion photoproduction"

description: Double polarization observables for $p\pi^0$ as a function of $\cos\vartheta$, invariant mass and $\phi^*$ for bins of the incident photon energy in the range of $E_\gamma$ = 800-950 MeV.
description: CBELSA/TAPS. Polarization observables in double neutral pion photoproduction

Individual contributions to the systematic uncertainty are given. These include:
 - sys,beampol: beam polarization (5% uncertainty)
 - sys,targetpol: target polarization (2% uncertainty)
 - sys,analysis: analysis (~1% uncertainty)
DOI: 10.17182/hepdata.137849.v1/t1
title: "Fig.1 (a), 7.7GeV, $F_{q}(M)$ of data and mixed events" of "Energy Dependence of Intermittency for Charged Hadrons in Au+Au Collisions at RHIC"

description: The scaled factorial moments, $F_{q}(M)$($q=$ 2-6), of identified charged hadrons ($h^{\pm}$) multiplicity in the most central (0-5\%) Au$+$Au collisions at $\sqrt{s_\mathrm{_{NN}}}$ = 7.7 GeV.
description: We report the first measurement of intermittency in Au$+$Au collisions at $\sqrt{s_\mathrm{_{NN}}}$ = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au$+$Au collisions and a decrease in the extracted scaling exponent ($\nu$) from peripheral to central collisions. The $\nu$ is consistent with a constant for different collisions energies in the mid-central (10-40\%) collisions. Moreover, the $\nu$ in the 0-5\% most central Au$+$Au collisions exhibits a non-monotonic energy dependence that reaches a minimum around $\sqrt{s_\mathrm{_{NN}}}$ = 27 GeV.
DOI: 10.17182/hepdata.137849.v1/t2
title: "Fig.1 (b), 19.6GeV, $F_{q}(M)$ of data and mixed events" of "Energy Dependence of Intermittency for Charged Hadrons in Au+Au Collisions at RHIC"

description: The scaled factorial moments, $F_{q}(M)$($q=$ 2-6), of identified charged hadrons ($h^{\pm}$) multiplicity in the most central (0-5\%) Au$+$Au collisions at $\sqrt{s_\mathrm{_{NN}}}$ = 19.6 GeV.
description: We report the first measurement of intermittency in Au$+$Au collisions at $\sqrt{s_\mathrm{_{NN}}}$ = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au$+$Au collisions and a decrease in the extracted scaling exponent ($\nu$) from peripheral to central collisions. The $\nu$ is consistent with a constant for different collisions energies in the mid-central (10-40\%) collisions. Moreover, the $\nu$ in the 0-5\% most central Au$+$Au collisions exhibits a non-monotonic energy dependence that reaches a minimum around $\sqrt{s_\mathrm{_{NN}}}$ = 27 GeV.
DOI: 10.17182/hepdata.137849.v1/t3
title: "Fig.1 (c), 39GeV, $F_{q}(M)$ of data and mixed events" of "Energy Dependence of Intermittency for Charged Hadrons in Au+Au Collisions at RHIC"

description: The scaled factorial moments, $F_{q}(M)$($q=$ 2-6), of identified charged hadrons ($h^{\pm}$) multiplicity in the most central (0-5\%) Au$+$Au collisions at $\sqrt{s_\mathrm{_{NN}}}$ = 39 GeV.
description: We report the first measurement of intermittency in Au$+$Au collisions at $\sqrt{s_\mathrm{_{NN}}}$ = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au$+$Au collisions and a decrease in the extracted scaling exponent ($\nu$) from peripheral to central collisions. The $\nu$ is consistent with a constant for different collisions energies in the mid-central (10-40\%) collisions. Moreover, the $\nu$ in the 0-5\% most central Au$+$Au collisions exhibits a non-monotonic energy dependence that reaches a minimum around $\sqrt{s_\mathrm{_{NN}}}$ = 27 GeV.
DOI: 10.17182/hepdata.137849.v1/t4
title: "Fig.1 (d), 200GeV, $F_{q}(M)$ of data and mixed events" of "Energy Dependence of Intermittency for Charged Hadrons in Au+Au Collisions at RHIC"

description: The scaled factorial moments, $F_{q}(M)$($q=$ 2-6), of identified charged hadrons ($h^{\pm}$) multiplicity in the most central (0-5\%) Au$+$Au collisions at $\sqrt{s_\mathrm{_{NN}}}$ = 200 GeV.
description: We report the first measurement of intermittency in Au$+$Au collisions at $\sqrt{s_\mathrm{_{NN}}}$ = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au$+$Au collisions and a decrease in the extracted scaling exponent ($\nu$) from peripheral to central collisions. The $\nu$ is consistent with a constant for different collisions energies in the mid-central (10-40\%) collisions. Moreover, the $\nu$ in the 0-5\% most central Au$+$Au collisions exhibits a non-monotonic energy dependence that reaches a minimum around $\sqrt{s_\mathrm{_{NN}}}$ = 27 GeV.