Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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2905 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6338 | 0.8277 | 0.7658 | [M:[0.9662, 1.1014, 0.9662, 0.8986, 0.7754, 0.7754], q:[0.7415, 0.2923], qb:[0.4155, 0.4831], phi:[0.5169]] | [M:[[4], [-12], [4], [12], [-3], [-3]], q:[[1], [-5]], qb:[[10], [2]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{1}$, ${ }M_{5}$, ${ }M_{6}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{1}$, ${ }M_{6}q_{1}\tilde{q}_{1}$ | ${}M_{4}\phi_{1}q_{2}^{2}$ | -2 | t^2.123 + 3*t^2.326 + t^2.696 + 2*t^2.899 + t^3.304 + t^3.471 + t^3.877 + t^4.043 + 2*t^4.246 + 4*t^4.449 + 6*t^4.652 + t^4.819 + 5*t^5.022 + 6*t^5.225 + t^5.391 + 3*t^5.594 + 2*t^5.63 + 4*t^5.797 - 2*t^6. + 2*t^6.167 + 2*t^6.203 + 5*t^6.37 + 4*t^6.572 + t^6.609 + t^6.739 + 8*t^6.775 + 4*t^6.942 + 7*t^6.978 + 6*t^7.145 + 10*t^7.348 + 2*t^7.515 + 8*t^7.551 + 6*t^7.717 - t^7.754 + 8*t^7.92 + 3*t^7.957 + 2*t^8.087 + 4*t^8.123 + 5*t^8.29 - 9*t^8.326 + 10*t^8.493 + t^8.529 + 8*t^8.696 + 2*t^8.862 - 2*t^8.899 + 2*t^8.935 - t^4.551/y - (2*t^6.877)/y + (2*t^7.449)/y + (4*t^7.652)/y + t^7.819/y + (5*t^8.022)/y + (8*t^8.225)/y + t^8.428/y + (3*t^8.594)/y + (3*t^8.63)/y + (4*t^8.797)/y - t^4.551*y - 2*t^6.877*y + 2*t^7.449*y + 4*t^7.652*y + t^7.819*y + 5*t^8.022*y + 8*t^8.225*y + t^8.428*y + 3*t^8.594*y + 3*t^8.63*y + 4*t^8.797*y | g1^5*t^2.123 + (3*t^2.326)/g1^3 + g1^12*t^2.696 + 2*g1^4*t^2.899 + t^3.304/g1^12 + g1^11*t^3.471 + t^3.877/g1^5 + g1^18*t^4.043 + 2*g1^10*t^4.246 + 4*g1^2*t^4.449 + (6*t^4.652)/g1^6 + g1^17*t^4.819 + 5*g1^9*t^5.022 + 6*g1*t^5.225 + g1^24*t^5.391 + 3*g1^16*t^5.594 + (2*t^5.63)/g1^15 + 4*g1^8*t^5.797 - 2*t^6. + 2*g1^23*t^6.167 + (2*t^6.203)/g1^8 + 5*g1^15*t^6.37 + 4*g1^7*t^6.572 + t^6.609/g1^24 + g1^30*t^6.739 + (8*t^6.775)/g1 + 4*g1^22*t^6.942 + (7*t^6.978)/g1^9 + 6*g1^14*t^7.145 + 10*g1^6*t^7.348 + 2*g1^29*t^7.515 + (8*t^7.551)/g1^2 + 6*g1^21*t^7.717 - t^7.754/g1^10 + 8*g1^13*t^7.92 + (3*t^7.957)/g1^18 + 2*g1^36*t^8.087 + 4*g1^5*t^8.123 + 5*g1^28*t^8.29 - (9*t^8.326)/g1^3 + 10*g1^20*t^8.493 + t^8.529/g1^11 + 8*g1^12*t^8.696 + 2*g1^35*t^8.862 - 2*g1^4*t^8.899 + (2*t^8.935)/g1^27 - t^4.551/(g1^2*y) - (2*t^6.877)/(g1^5*y) + (2*g1^2*t^7.449)/y + (4*t^7.652)/(g1^6*y) + (g1^17*t^7.819)/y + (5*g1^9*t^8.022)/y + (8*g1*t^8.225)/y + t^8.428/(g1^7*y) + (3*g1^16*t^8.594)/y + (3*t^8.63)/(g1^15*y) + (4*g1^8*t^8.797)/y - (t^4.551*y)/g1^2 - (2*t^6.877*y)/g1^5 + 2*g1^2*t^7.449*y + (4*t^7.652*y)/g1^6 + g1^17*t^7.819*y + 5*g1^9*t^8.022*y + 8*g1*t^8.225*y + (t^8.428*y)/g1^7 + 3*g1^16*t^8.594*y + (3*t^8.63*y)/g1^15 + 4*g1^8*t^8.797*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
1885 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | 0.616 | 0.7963 | 0.7736 | [M:[0.964, 1.108, 0.964, 0.892, 0.777], q:[0.741, 0.295], qb:[0.41, 0.482], phi:[0.518]] | t^2.115 + 2*t^2.331 + t^2.676 + 2*t^2.892 + t^3.324 + t^3.453 + t^3.669 + t^3.885 + t^4.014 + 2*t^4.23 + 3*t^4.446 + 3*t^4.662 + t^4.791 + 4*t^5.007 + 4*t^5.223 + t^5.352 + 3*t^5.568 + t^5.655 + 4*t^5.784 - t^4.554/y - t^4.554*y | detail |