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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933 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{1}M_{6}$ | 0.7226 | 0.8888 | 0.8131 | [M:[1.0234, 0.7968, 0.9766, 0.8437, 1.0, 0.9766], q:[0.5, 0.4766], qb:[0.5234, 0.6798], phi:[0.4551]] | [M:[[1, 0], [-1, -4], [-1, 0], [1, -4], [0, 0], [-1, 0]], q:[[0, 0], [-1, 0]], qb:[[1, 0], [0, 4]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$ | ${}$ | -3 | t^2.39 + t^2.531 + t^2.73 + 2*t^2.93 + t^3. + t^3.539 + t^4.225 + t^4.295 + 2*t^4.365 + t^4.435 + t^4.506 + t^4.781 + t^4.834 + t^4.904 + t^4.921 + t^4.975 + t^5.062 + t^5.121 + t^5.261 + 2*t^5.32 + t^5.444 + 2*t^5.461 + 2*t^5.66 + t^5.73 + 2*t^5.859 + t^5.93 - 3*t^6. - t^6.07 - t^6.141 + t^6.27 + t^6.469 - t^6.539 - t^6.61 + t^6.615 + t^6.685 + 2*t^6.756 + t^6.826 + 2*t^6.896 + t^6.955 + t^6.966 + t^7.025 + t^7.037 + t^7.079 + 2*t^7.096 + 2*t^7.154 + t^7.166 + t^7.171 + 3*t^7.225 + t^7.236 + 3*t^7.295 + t^7.312 + 2*t^7.365 + t^7.435 + t^7.452 - t^7.494 + t^7.506 + t^7.511 + t^7.593 - t^7.635 + t^7.652 + 2*t^7.711 + 2*t^7.764 - t^7.775 + t^7.792 + 2*t^7.834 + 2*t^7.851 + t^7.904 + 2*t^7.992 + 2*t^8.051 - t^8.104 + 2*t^8.191 - t^8.244 + 2*t^8.25 - t^8.32 + 2*t^8.373 - t^8.39 + t^8.444 + t^8.449 - t^8.461 + t^8.52 - 4*t^8.531 + 4*t^8.59 - t^8.601 + 3*t^8.66 - t^8.672 - t^8.713 + 2*t^8.789 + t^8.801 + t^8.871 - 8*t^8.93 + t^8.941 + t^8.983 - t^4.365/y - t^6.756/y - t^6.896/y - t^7.096/y - t^7.295/y + t^7.435/y + t^7.635/y + t^7.834/y + t^7.921/y + t^7.975/y + t^8.121/y + t^8.261/y + (2*t^8.32)/y + t^8.39/y + (2*t^8.461)/y + t^8.531/y + (2*t^8.66)/y + t^8.73/y + t^8.859/y + (3*t^8.93)/y - t^4.365*y - t^6.756*y - t^6.896*y - t^7.096*y - t^7.295*y + t^7.435*y + t^7.635*y + t^7.834*y + t^7.921*y + t^7.975*y + t^8.121*y + t^8.261*y + 2*t^8.32*y + t^8.39*y + 2*t^8.461*y + t^8.531*y + 2*t^8.66*y + t^8.73*y + t^8.859*y + 3*t^8.93*y | t^2.39/(g1*g2^4) + (g1*t^2.531)/g2^4 + t^2.73/g2^2 + (2*t^2.93)/g1 + t^3. + g2^4*t^3.539 + t^4.225/(g1^2*g2) + t^4.295/(g1*g2) + (2*t^4.365)/g2 + (g1*t^4.435)/g2 + (g1^2*t^4.506)/g2 + t^4.781/(g1^2*g2^8) + (g2^3*t^4.834)/g1 + g2^3*t^4.904 + t^4.921/g2^8 + g1*g2^3*t^4.975 + (g1^2*t^5.062)/g2^8 + t^5.121/(g1*g2^6) + (g1*t^5.261)/g2^6 + (2*t^5.32)/(g1^2*g2^4) + g2^7*t^5.444 + (2*t^5.461)/g2^4 + (2*t^5.66)/(g1*g2^2) + t^5.73/g2^2 + (2*t^5.859)/g1^2 + t^5.93/g1 - 3*t^6. - g1*t^6.07 - g1^2*t^6.141 + g2^2*t^6.27 + (g2^4*t^6.469)/g1 - g2^4*t^6.539 - g1*g2^4*t^6.61 + t^6.615/(g1^3*g2^5) + t^6.685/(g1^2*g2^5) + (2*t^6.756)/(g1*g2^5) + t^6.826/g2^5 + (2*g1*t^6.896)/g2^5 + t^6.955/(g1^2*g2^3) + (g1^2*t^6.966)/g2^5 + t^7.025/(g1*g2^3) + (g1^3*t^7.037)/g2^5 + g2^8*t^7.079 + (2*t^7.096)/g2^3 + (2*t^7.154)/(g1^3*g2) + (g1*t^7.166)/g2^3 + t^7.171/(g1^3*g2^12) + (3*t^7.225)/(g1^2*g2) + (g1^2*t^7.236)/g2^3 + (3*t^7.295)/(g1*g2) + t^7.312/(g1*g2^12) + (2*t^7.365)/g2 + (g1*t^7.435)/g2 + (g1*t^7.452)/g2^12 - (g2*t^7.494)/g1^2 + (g1^2*t^7.506)/g2 + t^7.511/(g1^2*g2^10) + (g1^3*t^7.593)/g2^12 - g2*t^7.635 + t^7.652/g2^10 + (2*t^7.711)/(g1^3*g2^8) + (2*g2^3*t^7.764)/g1^2 - g1^2*g2*t^7.775 + (g1^2*t^7.792)/g2^10 + (2*g2^3*t^7.834)/g1 + (2*t^7.851)/(g1*g2^8) + g2^3*t^7.904 + (2*g1*t^7.992)/g2^8 + (2*t^8.051)/(g1^2*g2^6) - (g2^5*t^8.104)/g1 + (2*t^8.191)/g2^6 - g1*g2^5*t^8.244 + (2*t^8.25)/(g1^3*g2^4) - t^8.32/(g1^2*g2^4) + (2*g2^7*t^8.373)/g1 - t^8.39/(g1*g2^4) + g2^7*t^8.444 + t^8.449/(g1^4*g2^2) - t^8.461/g2^4 + t^8.52/(g1^3*g2^2) - (4*g1*t^8.531)/g2^4 + (4*t^8.59)/(g1^2*g2^2) - (g1^2*t^8.601)/g2^4 + (3*t^8.66)/(g1*g2^2) - (g1^3*t^8.672)/g2^4 - g2^9*t^8.713 + (2*t^8.789)/g1^3 + (g1*t^8.801)/g2^2 + (g1^2*t^8.871)/g2^2 - (8*t^8.93)/g1 + (g1^3*t^8.941)/g2^2 + g2^11*t^8.983 - t^4.365/(g2*y) - t^6.756/(g1*g2^5*y) - (g1*t^6.896)/(g2^5*y) - t^7.096/(g2^3*y) - t^7.295/(g1*g2*y) + (g1*t^7.435)/(g2*y) + (g2*t^7.635)/y + (g2^3*t^7.834)/(g1*y) + t^7.921/(g2^8*y) + (g1*g2^3*t^7.975)/y + t^8.121/(g1*g2^6*y) + (g1*t^8.261)/(g2^6*y) + (2*t^8.32)/(g1^2*g2^4*y) + t^8.39/(g1*g2^4*y) + (2*t^8.461)/(g2^4*y) + (g1*t^8.531)/(g2^4*y) + (2*t^8.66)/(g1*g2^2*y) + t^8.73/(g2^2*y) + t^8.859/(g1^2*y) + (3*t^8.93)/(g1*y) - (t^4.365*y)/g2 - (t^6.756*y)/(g1*g2^5) - (g1*t^6.896*y)/g2^5 - (t^7.096*y)/g2^3 - (t^7.295*y)/(g1*g2) + (g1*t^7.435*y)/g2 + g2*t^7.635*y + (g2^3*t^7.834*y)/g1 + (t^7.921*y)/g2^8 + g1*g2^3*t^7.975*y + (t^8.121*y)/(g1*g2^6) + (g1*t^8.261*y)/g2^6 + (2*t^8.32*y)/(g1^2*g2^4) + (t^8.39*y)/(g1*g2^4) + (2*t^8.461*y)/g2^4 + (g1*t^8.531*y)/g2^4 + (2*t^8.66*y)/(g1*g2^2) + (t^8.73*y)/g2^2 + (t^8.859*y)/g1^2 + (3*t^8.93*y)/g1 |
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 |
---|---|---|---|---|---|---|---|---|---|
593 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{3}$ | 0.7215 | 0.8862 | 0.8142 | [M:[1.0, 0.8197, 1.0, 0.8197, 1.0], q:[0.5, 0.5], qb:[0.5, 0.6803], phi:[0.4549]] | 2*t^2.459 + t^2.73 + 3*t^3. + t^3.541 + 6*t^4.365 + 3*t^4.906 + 3*t^4.918 + 2*t^5.189 + t^5.446 + 4*t^5.459 + 3*t^5.73 - 2*t^6. - t^4.365/y - t^4.365*y | detail |