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Sharing Data Through Plots with Plotly by Alex Johnson

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Plotly is a web-based visualization and data analysis platform. Sharing Plotly plots in your dataverse creates a rich experience in which each user can interact with the data in whatever way best fits their needs: from zooming in and examining individual data points, to changing colors and styles, to importing the raw data into their favorite software environment for further analysis.

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Sharing Data Through Plots with Plotly by Alex Johnson

  1. 1. Sharing data through plots with Plotly Alex Johnson CTO, Plotly
  2. 2. A Plotly figure contains: • the data, in as raw a form as possible • a description of how to display that data • The figure is drawn fresh on every view • Viewers can edit the figure, download the data, or bring the whole figure into their favorite analysis language The goal: Share data so it’s accessible to all • Maintain the network of sources, acquisition/analysis/simulation scripts, related information, and references • Let each reader interact with the data in their own way • The figure is the most compact and meaningful representation of the data • Keep the data with the figure
  3. 3. An interactive article spin ‘‘flip’’ is accompanied by a nuclear spin with mI 1. The change in Bnuc associated s flip-flop transition is along the direction of exter- , taking into account the positive nuclear g factors nd As [2]. The cyclic repetition of the transition to T can thereby lead to a finite time-averaged ented along the external field. value of detuning where the S-T anticrossing denoted [see Fig. 1(b)], is a sensitive function for jBtotj 80 mT, providing a straightforward f measuring Bnuc within that range. To calibrate surement, the dependence of on external field de B0 is measured using the pulse sequence shown (c): The 0; 2 S state is first prepared at point P. A zed singlet in (1,1) is created by moving to point S g S) via point P0. The system is held at point S for S T2 then moved to point M and held there for est part of the cycle. The sequence is then repeated. S , rapid mixing of S and T states occurs. he system is moved to point M, the (1,1) charge l return to (0,2) only if the separated spins are in a onfiguration. The probability of being in the sin- e after time S thus appears as charge signal—the ce between the (1,1) and (0,2) charge states— by measuring the time-averaged QPC conduc- S [see Fig. 1(a)]. Figure 1(c) shows gS as a function nd VR with this pulse sequence applied. The field nce of this signal is shown in Fig. 1(d), which plots rated singlet state probability, PS, as a function of and electron Zeeman energies would prevent flip-flop pro- cesses [23]. We begin by examining the statistical polarization se- quence shown in Fig. 2(a). We first measure PS as a function of B0 and S, with S 100 ns, P 300 ns, P0 100 ns, M 32 s. These data, shown in Fig. 3(a), map out the S-T anticrossing in the limit of minimal measurement induced polarization (polarization is negli- gible for M > 30 s, as will be shown below). A steady- state nuclear polarization at B0 24 mT results in a shift in the position of , depending on the measurement time M, which determines the cycle period [Fig. 3(b)]. As M decreases, the position of moves to larger values of detuning, indicating an increase in the average Bnuc. For M > 30 s, the value of saturates to its unpolarized value. Values for Bnuc M can be extracted from calibrat- Adiabatic nuclear polarizationProbabilistic nuclear polarization Rapid Adiabatic Passage Slow Adiabatic Passage Prepare Singlet Rapid Adiabatic Passage, S-T+ evolution PS Prepare Singlet t= S t=0 Rapid Adiabatic Passage, Projection a) b) t= S t=0 1-PS Energy (0,2)S 0 (0,2)S T0 T+ T-Energy (0,2)S 0 (0,2)S T0 T+ T- Energy (0,2)S 0 (0,2)S T0 T+ T- Energy (0,2)S 0 (0,2)S T0 T+ T- Energy (0,2)S 0 (0,2)S T0 T+ T- S Energy (0,2)S 0 (0,2)S T0 T+ T- F FIG. 2 (color online). (a) Probabilistic nuclear polarization sequence. (b) Adiabatic nuclear polarization sequence (see text). ability diagram (see text). The bright signal at point M parallel to the 0 line is a result of Pauli-blocked 0; 2 charge transitions and reflects S-T mixing at (d) PS S 200 ns as a function of S and B0. The endent ‘‘spin funnel’’ corresponds to the S-T anti- position, S . 067601-2 https://plot.ly/~alex/484
  4. 4. Keep the data with the figure
  5. 5. Keep the data with the figure
  6. 6. EXTRAS Sources Ice cream plants Quandl:USDANASS/NASS_ICECREAMPRODUCTIONMEASUREDINPLANTS Ice cream gallons Quandl:USDANASS/NASS_ICECREAMPRODUCTIONMEASUREDINGALLONS US population Quandl:MWORTH/0_3 Extras AJPM: Ice Cream Illusions - Wansink et al. 2006 IC_dynamics.py Alex Johnson Dataverse: I scream, you scream! Sourced by JackParmer: Ice cream trend analysis JackParmer: The golden age of ice cream MattSundquist: Global ice cream demand The data and analysis network
  7. 7. Interact with the data your way
  8. 8. Interact with the data your way
  9. 9. Interact with the data your way
  10. 10. Plotly plots

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