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 |
---|---|---|---|---|---|---|---|---|---|
46458 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ | 0.5546 | 0.7066 | 0.7848 | [M:[0.8656, 1.1344, 0.7611, 0.9702], q:[0.9702, 0.5969], qb:[0.2687, 0.4328], phi:[0.4328]] | [M:[[2], [-2], [11], [-7]], q:[[-7], [6]], qb:[[-4], [1]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{4}$ | ${}M_{1}M_{2}$ | -1 | t^2.105 + t^2.283 + 2*t^2.597 + 2*t^2.911 + t^3.403 + t^3.895 + 2*t^4.209 + t^4.388 + t^4.566 + 3*t^4.702 + 2*t^4.88 + 2*t^5.015 + 4*t^5.194 + 4*t^5.508 + 3*t^5.821 - t^6. + t^6.179 + 2*t^6.314 + t^6.492 + t^6.671 + 3*t^6.806 + t^6.85 + 2*t^6.985 + 3*t^7.12 + 2*t^7.163 + 3*t^7.298 + 4*t^7.477 + 4*t^7.612 + 4*t^7.791 + 3*t^7.926 + 3*t^8.105 - 3*t^8.283 + 6*t^8.418 + t^8.462 - 4*t^8.597 + 4*t^8.732 + t^8.776 - 4*t^8.911 + t^8.954 - t^4.298/y - t^6.582/y - t^6.895/y - t^7.209/y + (2*t^7.388)/y + (3*t^7.702)/y + (2*t^7.88)/y + (3*t^8.015)/y + (3*t^8.194)/y + (5*t^8.508)/y + t^8.686/y + t^8.821/y - t^8.865/y - t^4.298*y - t^6.582*y - t^6.895*y - t^7.209*y + 2*t^7.388*y + 3*t^7.702*y + 2*t^7.88*y + 3*t^8.015*y + 3*t^8.194*y + 5*t^8.508*y + t^8.686*y + t^8.821*y - t^8.865*y | t^2.105/g1^3 + g1^11*t^2.283 + 2*g1^2*t^2.597 + (2*t^2.911)/g1^7 + t^3.403/g1^2 + g1^3*t^3.895 + (2*t^4.209)/g1^6 + g1^8*t^4.388 + g1^22*t^4.566 + (3*t^4.702)/g1 + 2*g1^13*t^4.88 + (2*t^5.015)/g1^10 + 4*g1^4*t^5.194 + (4*t^5.508)/g1^5 + (3*t^5.821)/g1^14 - t^6. + g1^14*t^6.179 + (2*t^6.314)/g1^9 + g1^5*t^6.492 + g1^19*t^6.671 + (3*t^6.806)/g1^4 + g1^33*t^6.85 + 2*g1^10*t^6.985 + (3*t^7.12)/g1^13 + 2*g1^24*t^7.163 + 3*g1*t^7.298 + 4*g1^15*t^7.477 + (4*t^7.612)/g1^8 + 4*g1^6*t^7.791 + (3*t^7.926)/g1^17 + (3*t^8.105)/g1^3 - 3*g1^11*t^8.283 + (6*t^8.418)/g1^12 + g1^25*t^8.462 - 4*g1^2*t^8.597 + (4*t^8.732)/g1^21 + g1^16*t^8.776 - (4*t^8.911)/g1^7 + g1^30*t^8.954 - (g1*t^4.298)/y - (g1^12*t^6.582)/y - (g1^3*t^6.895)/y - t^7.209/(g1^6*y) + (2*g1^8*t^7.388)/y + (3*t^7.702)/(g1*y) + (2*g1^13*t^7.88)/y + (3*t^8.015)/(g1^10*y) + (3*g1^4*t^8.194)/y + (5*t^8.508)/(g1^5*y) + (g1^9*t^8.686)/y + t^8.821/(g1^14*y) - (g1^23*t^8.865)/y - g1*t^4.298*y - g1^12*t^6.582*y - g1^3*t^6.895*y - (t^7.209*y)/g1^6 + 2*g1^8*t^7.388*y + (3*t^7.702*y)/g1 + 2*g1^13*t^7.88*y + (3*t^8.015*y)/g1^10 + 3*g1^4*t^8.194*y + (5*t^8.508*y)/g1^5 + g1^9*t^8.686*y + (t^8.821*y)/g1^14 - g1^23*t^8.865*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 |
---|
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 |
---|
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 |
---|
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 |
---|---|---|---|---|---|---|---|---|---|
46111 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ | 0.5532 | 0.705 | 0.7847 | [M:[0.857, 1.143, 0.7135], q:[1.0005, 0.571], qb:[0.286, 0.4285], phi:[0.4285]] | t^2.14 + t^2.144 + 2*t^2.571 + t^2.998 + t^3.002 + t^3.429 + t^3.856 + t^4.281 + t^4.284 + 2*t^4.287 + 2*t^4.711 + 3*t^4.715 + t^5.139 + 4*t^5.142 + t^5.145 + 2*t^5.569 + 2*t^5.573 + 2*t^5.997 - t^4.285/y - t^4.285*y | detail |