20 research outputs found
Data_Sheet_1_Embodiment and Humiliation Moderation of Neural Responses to Others' Suffering in Female Submissive BDSM Practitioners.docx
<p>Giving and receiving pain are common in the practice of BDSM (bondage-discipline, dominance-submission, and sadism-masochism). Playing a submissive role during BDSM practice weakens both the behavioral and neural empathic responses of female individuals to others' suffering, suggesting that long-term BDSM experience affects BDSM practitioners' empathic ability. This study further investigates whether physical restriction during BDSM practice also modulates individuals' neural responses to others' suffering. We measured neural responses to others' suffering by recording event-related potentials (ERPs) in female submissives while they viewed painful and neutral expressions in sexual sadistic/general social contexts under ball gag Blocking and Relaxed conditions. The neural responses recorded during 92–112 ms (N1), 132–172 ms (P2), 200–340 ms (N2), early late positive potential (LPP, 400–600 ms), and late LPP (700–1,000 ms) were included in the analyses. Compared to the relaxed condition, when a ball gag was used to prevent facial muscle movement and facial mimicry, the N1, early LPP, and late LPP responses neural responses to others' suffering were inhibited. The moderation effect of ball gag blocking on the N1 and early LPP amplitudes was positively correlated with the subjective feelings of facial muscle stillness, and the blocking moderation effect on the late LPP amplitudes was positively correlated with subjective feelings of humiliation. This study is the first neuropsychological investigation of the transient BDSM-related physical restriction effects on BDSM practitioners. These findings suggest that physical restriction (via a ball gag) during BDSM practices increases the wearer's facial muscle stillness and sense of humiliation. This physical restriction inhibits both early automatic responses and late controlled processes in response to the suffering of others.</p
Ca<sub>3</sub>Na<sub>4</sub>LiBe<sub>4</sub>B<sub>10</sub>O<sub>24</sub>F: A New Beryllium Borate with a Unique Beryl Borate <sub>∞</sub><sup>2</sup>[Be<sub>8</sub>B<sub>16</sub>O<sub>40</sub>F<sub>2</sub>] Layer Intrabridged by [B<sub>12</sub>O<sub>24</sub>] Groups
A novel
beryllium borate, Ca<sub>3</sub>Na<sub>4</sub>LiBe<sub>4</sub>B<sub>10</sub>O<sub>24</sub>F, has been discovered. It possesses a unique <sub>∞</sub><sup>2</sup>[Be<sub>8</sub>B<sub>16</sub>O<sub>40</sub>F<sub>2</sub>] layer composed
of two opposite parallel [Be<sub>4</sub>B<sub>4</sub>O<sub>12</sub>F]<sub>∞</sub> layers bridged with [B<sub>12</sub>O<sub>24</sub>] polyborates. The linkage of [B<sub>12</sub>O<sub>24</sub>] to other
structural units is first found in anhydrous borates. In the <sub>∞</sub><sup>2</sup>[Be<sub>8</sub>B<sub>16</sub>O<sub>40</sub>F<sub>2</sub>] layer, multiple
tunnels are arranged along different directions resided by the alkali
and alkaline-earth cations. The compound remains stable in an ambient
atmosphere from room temperature to the melting point at 830 °C
and melts incongruently
Structural Evolution in BaSn<sub>2</sub>F<sub>5</sub>X (X = Cl, Br, I): A Family of Alkaline Earth Metal Tin Mixed Halides
As
the first family of Sn-based alkaline earth metal mixed halides, three
new compounds, BaSn<sub>2</sub>F<sub>5</sub>X (X = Cl, Br, and I),
are synthesized by hydrothermal method. These compounds are crystallized
in the centrosymmetric space groups of <i>P</i>2<sub>1</sub>/<i>c</i>, <i>P</i>4/<i>nmm</i>, and <i>Pmma</i> for BaSn<sub>2</sub>F<sub>5</sub>Cl, BaSn<sub>2</sub>F<sub>5</sub>Br, and BaSn<sub>2</sub>F<sub>5</sub>I, respectively,
and their microscopic frameworks are all composed of the fundamental
structural unit [SnF<sub>4</sub>]<sup>2–</sup> and its derivatives
([SnF<sub>4</sub>Cl]<sup>3–</sup> and [SnF<sub>5</sub>]<sup>3–</sup> groups). Interestingly, the structures in BaSn<sub>2</sub>F<sub>5</sub>X are significantly changed from one-dimensional
(1D) to two-dimensional (2D) and then to 1D motifs as X varies from
Cl, Br, to I. Structural analysis combined with theoretical calculations
reveals that the structural diversities are caused by the difference
of ionic radius and electronegativity of X<sup>–</sup> anions
as well as the orientation of the lone-pair electrons on Sn<sup>2+</sup> cations. Moreover, the optical, electronic, and thermal properties
for these three compounds are determined. This work provides a representative
example to show how microscopic ions influence the structures, thus
in favor of the design for new mixed halides, a type of important
functional materials with many optoelectronic applications
Ca<sub>3</sub>Na<sub>4</sub>LiBe<sub>4</sub>B<sub>10</sub>O<sub>24</sub>F: A New Beryllium Borate with a Unique Beryl Borate <sub>∞</sub><sup>2</sup>[Be<sub>8</sub>B<sub>16</sub>O<sub>40</sub>F<sub>2</sub>] Layer Intrabridged by [B<sub>12</sub>O<sub>24</sub>] Groups
A novel
beryllium borate, Ca<sub>3</sub>Na<sub>4</sub>LiBe<sub>4</sub>B<sub>10</sub>O<sub>24</sub>F, has been discovered. It possesses a unique <sub>∞</sub><sup>2</sup>[Be<sub>8</sub>B<sub>16</sub>O<sub>40</sub>F<sub>2</sub>] layer composed
of two opposite parallel [Be<sub>4</sub>B<sub>4</sub>O<sub>12</sub>F]<sub>∞</sub> layers bridged with [B<sub>12</sub>O<sub>24</sub>] polyborates. The linkage of [B<sub>12</sub>O<sub>24</sub>] to other
structural units is first found in anhydrous borates. In the <sub>∞</sub><sup>2</sup>[Be<sub>8</sub>B<sub>16</sub>O<sub>40</sub>F<sub>2</sub>] layer, multiple
tunnels are arranged along different directions resided by the alkali
and alkaline-earth cations. The compound remains stable in an ambient
atmosphere from room temperature to the melting point at 830 °C
and melts incongruently
Experimental paradigm with factors gaze direction, agent’s ethnicity, and emotion.
<p><b><b><i>Note:</i></b><b> Between-subject variable  =  participant’s ethnicity.</b></b></p
Interaction effect of participant’s ethnicity, agent’s ethnicity, gaze direction, and emotion.
<p>Results refer to agents that show direct gaze (DIRECT). Top panel shows results for happiness, bottom panel shows results for anger. <i>Note:</i> Error bars indicate the 95% confidence interval. * <i>p</i><.05.</p
Nonlinear Optical Crystal Rb<sub>4</sub>Sn<sub>3</sub>Cl<sub>2</sub>Br<sub>8</sub>: Synthesis, Structure, and Characterization
A new
Sn-based halide compound, Rb<sub>4</sub>Sn<sub>3</sub>Cl<sub>2</sub>Br<sub>8</sub>, is synthesized by hydrothermal method. This
compound crystallizes in orthorhombic noncentrosymmetric space group
of <i>Cmc</i>2<sub>1</sub>, and the structure is composed
of one-dimensional [Sn<sub>4</sub>Cl<sub>2</sub>Br<sub>8</sub>]<sup>1</sup><sub>∞</sub> chains elongated in parallel to the <i>a</i>-axis. Interestingly, in the [Sn<sub>4</sub>Cl<sub>2</sub>Br<sub>8</sub>]<sup>1</sup><sub>∞</sub> chains the [SnBr<sub>5</sub>] and [SnClBr<sub>4</sub>] groups hold pyramidal configurations
which are found for the first time in Sn-based metal halides. Rb<sub>4</sub>Sn<sub>3</sub>Cl<sub>2</sub>Br<sub>8</sub> exhibits a high
thermal stability (up to 270 °C) and a relatively large bandgap
of 2.82 eV. This compound shows a phase-matchable powder second harmonic
generation response of 0.5 times of KH<sub>2</sub>PO<sub>4</sub> (KDP),
and is the first phase-matchable Sn-based halide nonlinear optical
material. The discovery of Rb<sub>4</sub>Sn<sub>3</sub>Cl<sub>2</sub>Br<sub>8</sub> will be beneficial to further phase-matchable nonlinear
optical materials exploration in Sn-based halides
Interaction effect of gaze direction, participant’s ethnicity, agent’s ethnicity, and emotion.
<p>Top panel shows results for happiness, bottom panel shows results for anger. <i>Note:</i> Error bars indicate the 95% confidence interval. * <i>p</i><.05; ** <i>p</i><.01.</p
ReBe<sub>2</sub>B<sub>5</sub>O<sub>11</sub> (Re = Y, Gd): Rare-Earth Beryllium Borates as Deep-Ultraviolet Nonlinear-Optical Materials
Two novel rare-earth beryllium borates <i>Re</i>Be<sub>2</sub>B<sub>5</sub>O<sub>11</sub> (<i>Re</i> = Y, Gd) have been discovered. These materials possess a unique
structural feature with a platelike infinite <sub>∞</sub><sup>2</sup>[Be<sub>2</sub>B<sub>5</sub>O<sub>11</sub>]<sup>3–</sup> superlayer, which is first found
in beryllium borates. The superlayer can be seen as sandwich-shaped
with <sub>∞</sub><sup>1</sup>[B<sub>4</sub>O<sub>8</sub>]<sup>4–</sup> chains linking up
with a <sub>∞</sub><sup>2</sup>[Be<sub>2</sub>BO<sub>5</sub>]<sup>3–</sup> sublayer above
and below via the B–O–Be bond. Each <sub>∞</sub><sup>2</sup>[Be<sub>2</sub>B<sub>5</sub>O<sub>11</sub>]<sup>3–</sup> layer is further connected to
the neighboring layer through <i>Re</i><sup>3+</sup> cations
coordinating with O atoms. Both of these two crystals have very short
cutoff wavelengths below 200 nm and exhibit relatively large nonlinear-optical
(NLO) effects, indicating their promising applications as good deep-UV
NLO crystals
First-Principles Design of a Deep-Ultraviolet Nonlinear-Optical Crystal from KBe<sub>2</sub>BO<sub>3</sub>F<sub>2</sub> to NH<sub>4</sub>Be<sub>2</sub>BO<sub>3</sub>F<sub>2</sub>
KBe<sub>2</sub>BO<sub>3</sub>F<sub>2</sub> (KBBF) is so far the sole nonlinear-optical (NLO) material
that can be practically applied in the deep-ultraviolet (DUV) region.
For the purpose of overcoming its layering tendency in crystal growth,
herein a computer-assisted material design system is employed to design
a new KBBF analogue, ammonia beryllium fluoroborate (NH<sub>4</sub>Be<sub>2</sub>BO<sub>3</sub>F<sub>2</sub>, ABBF). The first-principles
calculations demonstrate that ABBF possesses NLO properties very close
to those of KBBF, thus exhibiting good DUV NLO capability. Moreover,
owing to the relatively strong chemical binding between layers, ABBF
would have a better growth habit compared with KBBF. Upon synthesis,
ABBF would be a very promising DUV NLO material