مسٹر چرچل
بالآخر مسٹر چرچل کو بھی پیام اجل آگیا، وہ ا س صدی کی عظیم ترین شخصیتوں میں تھے، ان میں اتنے کمالات جمع تھے کہ مشکل ہی سے ایک انسان میں جمع ہوتے ہیں، وہ صحیح معنوں میں صاحب السیف و القلم بلکہ کچھ اس سے بھی زیادہ تھے، ایوان سیاست میں بے نظیر و مدبر، عرصۂ رزم میں جنگ آزما سپہ سالار میدان علم و ادب میں سحر طراز ادیب و خطیب، وہ اپنی قوم کے بہت بڑے محسن تھے، انھوں نے جتنی طویل مدت تک اپنے ملک و قوم کی خدمت کی اس کا موقع کم لیڈروں کو ملتا ہے، انھوں نے نوے سال کی عمر پائی اور ستر سال تک مسلسل کسی نہ کسی حیثیت سے خدمت کرتے رہے، وہ برطانوی قوم کے ناخدا تھے، انھوں نے ایسے نازک موقعوں پر اس کو ڈوبنے سے بچایا جب اس کی امید بہت کم رہ گئی تھی، گو وہ قدامت پرست طبقہ سے تعلق رکھتے تھے جس کا نقطہ نظر برطانوی شہنشاہیت کی توسیع و استحکام اور دنیا میں اس کی بالادستی تھا لیکن وہ اتنے بڑے آدمی تھے اور انھوں نے اپنی قوم کی اتنی گوناگوں خدمات انجام دیں کہ ان کی ذات دنیا کے لیڈروں کے لئے نمونہ ہے جس سے ان کو سبق حاصل کرنا چاہیے۔
(شاہ معین الدین ندوی،فروری ۱۹۶۵ء)
Medieval Punjab was amongst the first regions of South Asia to encounter the substantial impact of early Sufi mystics. This article aims to investigate the history of the Punjab from a Sufi perspective with particular focus on Chishtiya Sufism and its generous role in diverting the local community center of attention. For that, the prominent Chishti Sufi Dargahs of Baba Farid Ganj Shaker in Pakpattan is selected. The study tries to investigate Dargahs’ impact on the socio-cultural and religious set up of the Medieval Punjab. How did it influence another important religion of the region i.e. Sikh belief, paper tried to highlight this impact as well.
(M) x -CuTl-1223; M = Ni, Co, CoFe 2 O 4 , Cr, Al 2 O 3 , nanoparticles-superconductor composites were synthesized by solid-state reaction (ceramic method) and their infield (magnetic) superconducting properties were investigated. Structural, morphological and compositional analysis of these composites were carried by using X-rays diffraction (XRD) analysis, scanning electron microscopy (SEM) and energy dispersive X-ray spectroscopy (EDX), respectively. The infield transport measurements were carried out by resistance versus temperature (RT) measurements with small current ( ˷ 10 μA) by using four-probe technique with the help of physical properties measurement system (PPMS). Broadening in superconducting transition region was observed with increasing the external applied magnetic field (H) in all the samples, which was attributed to thermally activated flux flow (TAFF). Flux pinning strength was calculated by using TAFF model. The field dependent flux flow activation energy {U o (H)} of CuTl-1223 superconducting matrix was increased with addition of ferri-magnetic (CoFe 2 O 4 ) and antiferromagnetic (Cr) nanoparticles up to certain optimum level of concentration. The transition width (ΔT) of CuTl-1223 phase was decreased after addition of these nanoparticles. The enhancement in U o (H) and reduction in ΔT show improvement in flux pinning ability of CuTl- 1223 matrix with addition of CoFe 2 O 4 and Cr nanoparticles. The flux pinning strength of CuTl- 1223 phase was decreased with addition of ferromagnetic (Ni and Co) and non-magnetic (Al 2 O 3 ) nanoparticles. It was observed that U o (H) decreases and ΔT increases with the addition of these nanoparticles. The suppression in U o (H) with increasing magnetic field obeys the power law (U o = β H - a ) . The value of ‘a’ corresponds to the suppression rate of U o (H) with H. The decrease in ‘a’ with the addition of Cr, Co, and Al 2 O 3 nanoparticles showed that the decreasing rate of activation energy with increasing H is lowered with addition of these nanoparticles. Thus although the addition of Co and Al 2 O 3 in CuTl-1223 matrix decreases its flux pinning but their addition has lowered the suppression rate of U o (H) with H, which shows that the inclusion of these nanoparticles can make CuTl-1223 superconductor suitable for high field applications. In case of addition of CoFe 2 O 4 and Ni nanoparticles in CuTl-1223 superconductor, value of ‘a’ increases which indicates that lowering rate of activation energy increases with the rise in H. The transition width (ΔT) was increased with the rise in H, which shows TAFF takes place in the samples with small current. It was observed that broadening in ΔT with ‘H’ obeys a power law (ΔT = ΔT o + CH n ) where ΔT o is the transition width in absence of applied field.