271 research outputs found

    Molecular cytogenetic aberrations in patients with multiple myeloma studied by interphase fluorescence in situ hybridization

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    Background: Multiple myeloma (MM) is an incurable hematological disorder characterized by the accumulation of malignant plasma cells within the bone marrow (BM). The clinical heterogeneity of MM is dictated by the cytogenetic aberrations present in the clonal plasma cells (PCs). Cytogenetic studies in MM are hampered by the hypoproliferative nature of plasma cells in MM. Therefore, fluorescence in situ hybridization (FISH) analysis combined with magnetic-activated cell sorting (MACS) is an attractive alternative for evaluation of numerical and structural chromosomal changes in MM. Methods: Interphase FISH studies with three different specific probes for the regions containing 13q14.3 (D13S319), 14q32 (IGHC/IGHV) and 1q12(CEP1 ) were performed in 48 MM patients. Interphase FISH studies with LSI IGH/CCND1, LSI IGH/FGFR3, and LSI IGH/MAF probes were used to detect t(11;14)(q13;q32), t(4;14)(p16;q32), and t(14;16)(q32;q23) in patients with 14q32 rearrangement. Results: Molecular cytogenetic aberrations were found in 40 (83.3%) of the 48 MM patients. 13 patients (27.1%) simultaneously had 13q deletion/monosomy 13 [del(13q14)], illegitimate IGH rearrangement and chromosome 1 abnormality. Del(13q14) was detected in 21 cases (43.7%), and illegitimate IGH rearrangements in 29 (60.4%) including 6 with t(11;14) and 5 with t(4;14). None of 9 patients with illegitimate IGH rearrangements and without t(11;14) or t(4;14) we detected had t(14;16) (q32;q23). 24 of the 48 MM patients (50%) had chromosome 1 abnormalities. Among 21 patients with del(13q14), 15 patients had Amp1q12;16 had IgH rearrangements. Whereas, among 27 cases without del(13q14), 8 had Amp1q12; 13 had IgH rearrangements. There was a strong association between del(13q14) and Amp1q12(c2 = 8.26, Ρ€ < 0.01), and between del(13q14) and IgH rearrangement(c2 = 3.88, p < 0.05). Conclusion: 13q deletion/monosomy 13, IGH rearrangement and chromosome 1 abnormality are frequent in MM. They are not randomly distributed, but strongly interconnected. Interphase FISH technique combined with MACS using CD138-specific antibody is a highly sensitive technique at detecting molecular cytogenetic aberrations in MM.ОбоснованиС: мноТСствСнная ΠΌΠΈΠ΅Π»ΠΎΠΌΠ° (MM) β€” Π½Π΅ΠΈΠ·Π»Π΅Ρ‡ΠΈΠΌΠΎΠ΅ гСматологичСскоС Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠ΅, Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ΠΈΠ·ΠΈΡ€ΡƒΡŽΡ‰Π΅Π΅ΡΡ Π½Π°ΠΊΠΎΠΏΠ»Π΅Π½ΠΈΠ΅ΠΌ злокачСствСнных плазматичСских ΠΊΠ»Π΅Ρ‚ΠΎΠΊ Π² костном ΠΌΠΎΠ·Π³Π΅ (КM). ΠšΠ»ΠΈΠ½ΠΈΡ‡Π΅ΡΠΊΠ°Ρ Π³Π΅Ρ‚Π΅Ρ€ΠΎΠ³Π΅Π½Π½ΠΎΡΡ‚ΡŒ MM опрСдСляСтся цитогСнСтичСскими абСррациями, ΠΏΡ€ΠΈΡΡƒΡ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠΌΠΈ Π² ΠΊΠ»ΠΎΠ½Π΅ плазматичСских ΠΊΠ»Π΅Ρ‚ΠΎΠΊ (ПК). ЦитогСнСтичСскиС исслСдования MM ослоТнСны Π³ΠΈΠΏΠΎΠΏΡ€ΠΎΠ»ΠΈΡ„Π΅Ρ€Π°Ρ‚ΠΈΠ²Π½Ρ‹ΠΌΠΈ особСнностями ПК. Π’ связи с этим флуорСсцСнтная гибридизация in situ (FISH) Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠΈ с сортировкой ΠΊΠ»Π΅Ρ‚ΠΎΠΊ, Π°ΠΊΡ‚ΠΈΠ²ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹ΠΌΠΈ полями (MACS) прСдставляСтся достойной Π°Π»ΡŒΡ‚Π΅Ρ€Π½Π°Ρ‚ΠΈΠ²ΠΎΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌ ΠΎΡ†Π΅Π½ΠΊΠΈ Ρ‚ΠΎΡ‡Π΅Ρ‡Π½Ρ‹Ρ… ΠΈ структурных ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ хромосом ΠΏΡ€ΠΈ MM. ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π°Π·Π½Ρ‹Π΅ исслСдования ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ FISH с использованиСм Ρ‚Ρ€Π΅Ρ… Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… спСцифичСских Π·ΠΎΠ½Π΄ΠΎΠ² для участков, содСрТащих 13q14.3 (D13S319), 14q32 (IGHC/IGHV) ΠΈ 1q12(CEP1), ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Ρƒ 48 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… с MM. Π˜Π½Ρ‚Π΅Ρ€Ρ„Π°Π·Π½Ρ‹Π΅ исслСдования ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ FISH с использованиСм Π·ΠΎΠ½Π΄ΠΎΠ² LSI IGH/CCND1, LSI IGH/FGFR3 ΠΈ LSI IGH/MAF примСняли для Π΄Π΅Ρ‚Π΅ΠΊΡ†ΠΈΠΈ t(11;14)(q13;q32), t(4;14)(p16;q32), ΠΈ t(14;16)(q32;q23) Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с пСрСстройкой 14q32. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹: молСкулярныС цитогСнСтичСскиС Π°Π±Π΅Ρ€Ρ€Π°Ρ†ΠΈΠΈ выявляли Ρƒ 40 (83,3%) ΠΈΠ· 48 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… с MM. Π£ 13 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² (27,1%) ΠΎΠ΄Π½ΠΎΠ²Ρ€Π΅ΠΌΠ΅Π½Π½ΠΎ ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ 13q дСлСция/моносомия 13 [del(13q14)], аномальная пСрСстройка IGH ΠΈ аномалия хромосомы 1. Del(13q14) Π΄Π΅Ρ‚Π΅ΠΊΡ‚ΠΈΡ€ΠΎΠ²Π°Π»ΠΈ Π² 21 случаС (43,7%), Π° Π°Π½ΠΎΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ пСрСстройки IGH β€” Π² 29 (60,4%), Π² Ρ‚ΠΎΠΌ числС Ρƒ 6 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с t(11;14) ΠΈ 5 с t(4;14). Ни Ρƒ ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΈΠ· 9 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… с Π°Π½ΠΎΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ пСрСстройками IGH ΠΈ Π±Π΅Π· t(11;14) ΠΈΠ»ΠΈ t(4;14) Π½Π΅ выявляли Ρ‚Ρ€Π°Π½ΡΠ»ΠΎΠΊΠ°Ρ†ΠΈΡŽ t(14;16) (q32;q23). Π£ 24 ΠΈΠ· 48 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с MM (50%) опрСдСляли Π°Π½ΠΎΠΌΠ°Π»ΠΈΠΈ хромосомы 1. Π’ Π³Ρ€ΡƒΠΏΠΏΠ΅ ΠΈΠ· 21 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… с del(13q14) Π² 15 случаях имСлись пСрСстройки IgH Amp1q12;16. Π’ Ρ‚ΠΎ ΠΆΠ΅ врСмя ΠΈΠ· 27 случаСв Π±Π΅Π· del(13q14) Ρƒ 8 ΡΠΎΠ΄Π΅Ρ€ΠΆΠ°Π»ΠΈΡΡŒ Amp1q12; Π² 13 случаях ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»ΠΈ пСрСстройки IgH. ВыявлСна взаимосвязь ΠΌΠ΅ΠΆΠ΄Ρƒ del(13q14) ΠΈ Amp1q12(Ο‡2 = 8,26, p < 0,01) ΠΈ ΠΌΠ΅ΠΆΠ΄Ρƒ del(13q14) ΠΈ пСрСстройками IgH (Ο‡2 = 3,88, p < 0,05). Π’Ρ‹Π²ΠΎΠ΄Ρ‹: 13q Π΄Π΅Π»Π΅Ρ†ΠΈΡŽ/моносомию 13, пСрСстройку IGH ΠΈ аномалию хромосомы 1 часто ΠΎΡ‚ΠΌΠ΅Ρ‡Π°ΡŽΡ‚ ΠΏΡ€ΠΈ MM, ΠΏΡ€ΠΈΡ‡Π΅ΠΌ ΠΈΡ… распрСдСлСниС Π½Π΅ случайно ΠΈ тСсно взаимосвязано. Π˜Π½Ρ‚Π΅Ρ€Ρ„Π°Π·Π½Ρ‹ΠΉ Π°Π½Π°Π»ΠΈΠ· FISH Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠΈ с MACS с использованиСм CD138-спСцифичных Π°Π½Ρ‚ΠΈΡ‚Π΅Π» являСтся Π²Ρ‹ΡΠΎΠΊΠΎΡ‡ΡƒΠ²ΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π΄Π΅Ρ‚Π΅ΠΊΡ†ΠΈΠΈ молСкулярных цитогСнСтичСских Π°Π±Π΅Ρ€Ρ€Π°Ρ†ΠΈΠΉ ΠΏΡ€ΠΈ MM

    Early Detection of t(8;21) Chromosomal Translocations During Treatment of PML-RARA Positive Acute Promyelocytic Leukemia: A Case Study

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    Here we describe a female patient who developed acute promyelocytic leukemia (APL) characterized by t(l5;17) translocation at diagnosis. The patient began treatment with all-trans retinoic acid (ATRA) + chemotherapy. During follow up, the patient was found to be negative for the t(15;17) transcript after 3 months of therapy which remained undetectable, thereafter. However, the emergence of a small clone with a t(8;21) abnormality was observed in the bone marrow and peripheral blood (PB) cells between 3 and 18 months following treatment initiation. The abnormal translocation observed in PB cells obtained at 3 months was detected after the second cycle of consolidation therapy and reappeared at 15 months during maintenance treatment, a period without ATRA. Although based on a single case, we conclude that genetic screening of multiple translocations in AML patients should be requested to allow early identification of other emerging clones during therapy that may manifest clinically following treatment

    Distortion in a 7xxx aluminum alloy during liquid phase sintering

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    The distortion in a sintered 7xxx aluminum alloy, Al-7Zn-2.5Mg-1Cu (wt. pct), has been investigated by sintering three rectangular bars in each batch at 893 K (620 Β°C) for 0 to 40 minutes in nitrogen, followed by air or furnace cooling. They were placed parallel to each other, equally spaced apart at 2 mm, with their long axes being perpendicular to the incoming nitrogen flow. Pore evolution in each sample during isothermal sintering was examined metallographically. The compositional changes across sample mid-cross section and surface layers were analyzed using energy dispersive X-ray spectroscopy and X-ray photoelectron spectroscopy depth profiling, respectively. The two outer samples bent toward the middle one, while the middle sample was essentially distortion free after sintering. The distortion in the outer samples was a result of differential shrinkage between their outer and inner surfaces during isothermal sintering. The porous outer surface showed an enrichment of oxygen around the large pores as well as lower magnesium and zinc contents than the interior and inner surface of the same sample, while the inner surface was distinguished by the presence of AlN. The differential shrinkage was caused by different oxygen contents in local sintering atmosphere and unbalanced loss of magnesium and zinc between the outer and inner surfaces

    Direct Measurements of the Branching Fractions for D0β†’Kβˆ’e+Ξ½eD^0 \to K^-e^+\nu_e and D0β†’Ο€βˆ’e+Ξ½eD^0 \to \pi^-e^+\nu_e and Determinations of the Form Factors f+K(0)f_{+}^{K}(0) and f+Ο€(0)f^{\pi}_{+}(0)

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    The absolute branching fractions for the decays D0β†’Kβˆ’e+Ξ½eD^0 \to K^-e ^+\nu_e and D0β†’Ο€βˆ’e+Ξ½eD^0 \to \pi^-e^+\nu_e are determined using 7584Β±198Β±3417584\pm 198 \pm 341 singly tagged DΛ‰0\bar D^0 sample from the data collected around 3.773 GeV with the BES-II detector at the BEPC. In the system recoiling against the singly tagged DΛ‰0\bar D^0 meson, 104.0Β±10.9104.0\pm 10.9 events for D0β†’Kβˆ’e+Ξ½eD^0 \to K^-e ^+\nu_e and 9.0Β±3.69.0 \pm 3.6 events for D0β†’Ο€βˆ’e+Ξ½eD^0 \to \pi^-e^+\nu_e decays are observed. Those yield the absolute branching fractions to be BF(D0β†’Kβˆ’e+Ξ½e)=(3.82Β±0.40Β±0.27)BF(D^0 \to K^-e^+\nu_e)=(3.82 \pm 0.40\pm 0.27)% and BF(D0β†’Ο€βˆ’e+Ξ½e)=(0.33Β±0.13Β±0.03)BF(D^0 \to \pi^-e^+\nu_e)=(0.33 \pm 0.13\pm 0.03)%. The vector form factors are determined to be ∣f+K(0)∣=0.78Β±0.04Β±0.03|f^K_+(0)| = 0.78 \pm 0.04 \pm 0.03 and ∣f+Ο€(0)∣=0.73Β±0.14Β±0.06|f^{\pi}_+(0)| = 0.73 \pm 0.14 \pm 0.06. The ratio of the two form factors is measured to be ∣f+Ο€(0)/f+K(0)∣=0.93Β±0.19Β±0.07|f^{\pi}_+(0)/f^K_+(0)|= 0.93 \pm 0.19 \pm 0.07.Comment: 6 pages, 5 figure

    Measurements of J/psi Decays into 2(pi+pi-)eta and 3(pi+pi-)eta

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    Based on a sample of 5.8X 10^7 J/psi events taken with the BESII detector, the branching fractions of J/psi--> 2(pi+pi-)eta and J/psi-->3(pi+pi-)eta are measured for the first time to be (2.26+-0.08+-0.27)X10^{-3} and (7.24+-0.96+-1.11)X10^{-4}, respectively.Comment: 11 pages, 6 figure

    BESII Detector Simulation

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    A Monte Carlo program based on Geant3 has been developed for BESII detector simulation. The organization of the program is outlined, and the digitization procedure for simulating the response of various sub-detectors is described. Comparisons with data show that the performance of the program is generally satisfactory.Comment: 17 pages, 14 figures, uses elsart.cls, to be submitted to NIM

    Measurement of branching fractions for the inclusive Cabibbo-favored ~K*0(892) and Cabibbo-suppressed K*0(892) decays of neutral and charged D mesons

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    The branching fractions for the inclusive Cabibbo-favored ~K*0 and Cabibbo-suppressed K*0 decays of D mesons are measured based on a data sample of 33 pb-1 collected at and around the center-of-mass energy of 3.773 GeV with the BES-II detector at the BEPC collider. The branching fractions for the decays D+(0) -> ~K*0(892)X and D0 -> K*0(892)X are determined to be BF(D0 -> \~K*0X) = (8.7 +/- 4.0 +/- 1.2)%, BF(D+ -> ~K*0X) = (23.2 +/- 4.5 +/- 3.0)% and BF(D0 -> K*0X) = (2.8 +/- 1.2 +/- 0.4)%. An upper limit on the branching fraction at 90% C.L. for the decay D+ -> K*0(892)X is set to be BF(D+ -> K*0X) < 6.6%

    Study of J/Οˆβ†’Ο‰K+Kβˆ’J/\psi \to \omega K^+K^-

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    New data are presented on J/Οˆβ†’Ο‰K+Kβˆ’J/\psi \to \omega K^+K^- from a sample of 58M J/ψJ/\psi events in the upgraded BES II detector at the BEPC. There is a conspicuous signal for f0(1710)β†’K+Kβˆ’f_0(1710) \to K^+K^- and a peak at higher mass which may be fitted with f2(2150)β†’KKΛ‰f_2(2150) \to K\bar K. From a combined analysis with ωπ+Ο€βˆ’\omega \pi ^+ \pi ^- data, the branching ratio BR(f0(1710)→ππ)/BR(f0(1710)β†’KKΛ‰)BR(f_0(1710)\to\pi\pi)/BR(f_0(1710) \to K\bar K) is <0.11< 0.11 at the 95% confidence level.Comment: 11 pages, 5 figures. Submitted to Phys. Lett.

    Measurements of the Mass and Full-Width of the Ξ·c\eta_c Meson

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    In a sample of 58 million J/ψJ/\psi events collected with the BES II detector, the process J/Οˆβ†’Ξ³Ξ·c\psi\to\gamma\eta_c is observed in five different decay channels: Ξ³K+Kβˆ’Ο€+Ο€βˆ’\gamma K^+K^-\pi^+\pi^-, Ξ³Ο€+Ο€βˆ’Ο€+Ο€βˆ’\gamma\pi^+\pi^-\pi^+\pi^-, Ξ³KΒ±KS0Ο€βˆ“\gamma K^\pm K^0_S \pi^\mp (with KS0β†’Ο€+Ο€βˆ’K^0_S\to\pi^+\pi^-), γϕϕ\gamma \phi\phi (with Ο•β†’K+Kβˆ’\phi\to K^+K^-) and Ξ³ppΛ‰\gamma p\bar{p}. From a combined fit of all five channels, we determine the mass and full-width of Ξ·c\eta_c to be mΞ·c=2977.5Β±1.0(stat.)Β±1.2(syst.)m_{\eta_c}=2977.5\pm1.0 ({stat.})\pm1.2 ({syst.}) MeV/c2c^2 and Γηc=17.0Β±3.7(stat.)Β±7.4(syst.)\Gamma_{\eta_c} = 17.0\pm3.7 ({stat.})\pm7.4 ({syst.}) MeV/c2c^2.Comment: 9 pages, 2 figures and 4 table. Submitted to Phys. Lett.

    Search for the Lepton Flavor Violation Processes J/Οˆβ†’J/\psi \to ΞΌΟ„\mu\tau and eΟ„e\tau

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    The lepton flavor violation processes J/Οˆβ†’ΞΌΟ„J/\psi \to \mu\tau and eΟ„e\tau are searched for using a sample of 5.8Γ—107\times 10^7 J/ψJ/\psi events collected with the BESII detector. Zero and one candidate events, consistent with the estimated background, are observed in J/Οˆβ†’ΞΌΟ„,Ο„β†’eΞ½Λ‰eΞ½Ο„J/\psi \to \mu\tau, \tau\to e\bar\nu_e\nu_{\tau} and J/Οˆβ†’eΟ„,Ο„β†’ΞΌΞ½Λ‰ΞΌΞ½Ο„J/\psi\to e\tau, \tau\to\mu\bar\nu_{\mu}\nu_{\tau} decays, respectively. Upper limits on the branching ratios are determined to be Br(J/Οˆβ†’ΞΌΟ„)<2.0Γ—10βˆ’6Br(J/\psi\to\mu\tau)<2.0 \times 10^{-6} and Br(J/Οˆβ†’eΟ„)<8.3Γ—10βˆ’6Br(J/\psi \to e\tau) < 8.3 \times10^{-6} at the 90% confidence level (C.L.).Comment: 9 pages, 2 figure
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